theory perspective on machine learning for jets · 2021. 6. 3. · jesse thaler (mit) — theory...
TRANSCRIPT
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Jets and their Substructure from LHC Data, CERN-TH Virtual Workshop — June 3, 2021
Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Jesse Thaler
Theory Perspective on
Machine Learning for Jets
[http://iaifi.org, MIT News Announcement]
The NSF AI Institute for Artificial Intelligenceand Fundamental Interactions (IAIFI)
Advance physics knowledge — from the smallest building blocks of nature
to the largest structures in the universe — and galvanize AI research innovation
“eye-phi”
2Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
3Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Machine learning that incorporatesfirst principles, best practices, and domain knowledge
from fundamental physics
Symmetries, conservation laws, scaling relations, limiting behaviors, locality, causality,unitarity, gauge invariance, entropy, least action, factorization, unit tests,
exactness, systematic uncertainties, reproducibility, verifiability, …
AI2: Ab Initio Artificial Intelligence
4Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Confronting the Black Box
How do we develop robust machine learning for jet analyses?
5Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Likelihood Ratio TrickKey example of simulation-based inference
[see e.g. Cranmer, Pavez, Louppe, arXiv 2015; D’Agnolo, Wulzer, PRD 2019;simulation-based inference in Cranmer, Brehmer, Louppe, PNAS 2020;
relation to f-divergences in Nguyen, Wainwright, Jordan, AoS 2009; Nachman, JDT, arXiv 2021]
Learnable Function:
Training Data: Finite samples P and Q
Goal: Estimate p(x) / q(x)
f(x) parametrized by, e.g., neural networks
−minf(x)
L =
Zdx p(x) log
p(x)
q(x)<latexit sha1_base64="DHXBjqaYO+bfMooFpxGVp6lB6cI=">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</latexit><latexit sha1_base64="DHXBjqaYO+bfMooFpxGVp6lB6cI=">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</latexit><latexit sha1_base64="DHXBjqaYO+bfMooFpxGVp6lB6cI=">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</latexit><latexit sha1_base64="TU7q4dQBpc+LJp2rM/pH2uS50uM=">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</latexit>
Loss Function(al):
Asymptotically:
Kullback–Leibler divergence
argminf(x)
L =p(x)
q(x)<latexit sha1_base64="C44EPfIX41lNtDowReWFHN5q4Ug=">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</latexit><latexit sha1_base64="C44EPfIX41lNtDowReWFHN5q4Ug=">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</latexit><latexit sha1_base64="C44EPfIX41lNtDowReWFHN5q4Ug=">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</latexit><latexit sha1_base64="aV3VBbPgU5blfbcq1YETF1NKiLY=">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</latexit>
Likelihood ratio
L = −
⌦
log f(x)↵
P+
⌦
f(x)− 1↵
Q<latexit sha1_base64="/BAofgnPH6B4QebhXUNq+8pNlqE=">AAAC73iclVLLahsxFNVMX6n7ctrushE1hZQmZjR1/FgUTLPpogsH6sTgGYxG1kxENJqppCk1g7pt/6C7kG0/KT+QD8gXRJ5JoHZKoRcuHM69557LlaKcM6U979xx79y9d//BxsPGo8dPnj5rbj4/VFkhCR2TjGdyEmFFORN0rJnmdJJLitOI06PoZH9ZP/pKpWKZ+KwXOQ1TnAgWM4K1pWbNy0/wPdyFQcSSgGORcAoDniWwDKrZU5lEYem19zw06KIdr+1VsXPDmHj72xtTy2Uln60pbTdCtRL1ukvlYND3Ud+MDHy74vt/lrsQ/ct20O/6nW6l7iG/GuP3Ou865sDMmq2bofA2QNegNXwJqhjNmhfBPCNFSoUmHCs1RV6uwxJLzQinphEUiuaYnOCETi0UOKUqLKt1DHxtmTmMM2lTaFixfypKnCq1SCPbmWJ9rNZrS/JvtWmh435YMpEXmgpSG8UFhzqDy4eGcyYp0XxhASaS2V0hOcYSE22/w4pLTBcizU3DHgatn+E2OPTbyGujg05r+KG+ENgAW+AV2AYI9MAQfAQjMAbEmTjfnR/OT/eL+8s9dc/qVte51rwAK+H+vgJwPt0k</latexit><latexit sha1_base64="/BAofgnPH6B4QebhXUNq+8pNlqE=">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</latexit><latexit sha1_base64="/BAofgnPH6B4QebhXUNq+8pNlqE=">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</latexit><latexit sha1_base64="kPIkJdH6omNFCZSl9SSaGcCTYJg=">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</latexit>
Many QCD/collider/jet problemscan be expressed in this form!
[see e.g. Cranmer, Pavez, Louppe, arXiv 2015; D’Agnolo, Wulzer, PRD 2019;simulation-based inference in Cranmer, Brehmer, Louppe, PNAS 2020;
relation to f-divergences in Nguyen, Wainwright, Jordan, AoS 2009; Nachman, JDT, arXiv 2021]
Many QCD/collider/jet problemscan be expressed in this form!Likelihood Ratio Trick
Key example of simulation-based inference
6Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Asymptotically, same structure as Lagrangian mechanics!
Action:
Lagrangian:
Euler-Lagrange: Solution:
L =
ZdxL(x)
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∂L
∂f= 0
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f(x) =p(x)
q(x)<latexit sha1_base64="quzVQzouxbo/tOnoZlw/ZCJVKpE=">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</latexit><latexit sha1_base64="quzVQzouxbo/tOnoZlw/ZCJVKpE=">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</latexit><latexit sha1_base64="quzVQzouxbo/tOnoZlw/ZCJVKpE=">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</latexit><latexit sha1_base64="htVSx2ZZujuo2Hdt9ibMaWlHcBA=">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</latexit>
L(x) = −p(x) log f(x) + q(x)�
f(x)− 1�
<latexit sha1_base64="K298pScNYU/Ys1xSLKz/x92RmiM=">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</latexit><latexit sha1_base64="K298pScNYU/Ys1xSLKz/x92RmiM=">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</latexit><latexit sha1_base64="K298pScNYU/Ys1xSLKz/x92RmiM=">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</latexit><latexit sha1_base64="CIzs/gC4UpWwhuj1TBR+6hF4fYI=">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</latexit>
Requires shift in theoretical focus from solving problems to specifying problems
7Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
“What is the machine learning?”
For this loss function, an estimate of the likelihood ratio derived from sampled data and regularized by the
network architecture and training paradigm
“But where’s the physics?!”
In the choice of loss function, data samples,network architecture, and training paradigm
“…”
8Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
[h/t David Kaiser, MIT SERC; Suresh, Guttag, arXiv 2019]
(a) Data Generation
(b) Model Building and Implementation
1. Historical bias arises when there is a misalignment be-tween world as it is and the values or objectives to beencoded and propagated in a model. It is a normative con-cern with the state of the world, and exists even given per-fect sampling and feature selection.
2. Representation bias arises while defining and samplinga development population. It occurs when the develop-ment population under-represents, and subsequently failsto generalize well, for some part of the use population.
3. Measurement Bias arises when choosing and measur-ing features and labels to use; these are often proxies forthe desired quantities. The chosen set of features and la-bels may leave out important factors or introduce group-or input-dependent noise that leads to differential perfor-mance.
4. Aggregation bias arises during model construction, whendistinct populations are inappropriately combined. Inmany applications, the population of interest is heteroge-neous and a single model is unlikely to suit all subgroups.
5. Evaluation bias occurs during model iteration and evalu-ation. It can arise when the testing or external benchmarkpopulations do not equally represent the various parts ofthe use population. Evaluation bias can also arise from theuse of performance metrics that are not appropriate for theway in which the model will be used.
6. Deployment Bias occurs after model deployment, whena system is used or interpreted in inapppropriate ways.
Many Reasons to be Wary! “A Framework for Understanding Unintended Consequences of Machine Learning”
For collider physics, “bias” ≈ “systematic uncertainty”
9Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Machine Learning for Jet Substructure
How can we leverage theory to advance machine learning for jets?
Jets from fragmentation
of quarks and gluons
10Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
My (Evolving) Perspective
Examples below are representative, not exhaustive; apologies![see HEPML-LivingReview for extensive bibliography]
When striving for “interpretable machine learning”we are essentially hoping that likelihood ratios can beapproximated via theoretically well-motivated forms
We can impose theoretical priors by judicious choice ofnetwork architecture that captures the underlying
structures and symmetries of our problem
Machine learning methods can only be as robust and reliableas the data samples used for training
We are making progress towards uncertainty quantification,using more elaborate loss functions and training paradigms
11Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
When striving for “interpretable machine learning”we are essentially hoping that likelihood ratios can beapproximated via theoretically well-motivated forms
We can impose theoretical priors by judicious choice ofnetwork architecture that captures the underlying
structures and symmetries of our problem
Machine learning methods can only be as robust and reliableas the data samples used for training
We are making progress towards uncertainty quantification,using more elaborate loss functions and training paradigms
12Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Compute Likelihood Ratios Directly?Yes, you can! And if you have enough calculational power, you should!
Shower Deconstruction Color Singlet Identification
Challenge is that in most cases, best estimate of likelihood ratiocomes from complex simulations with no closed form expression
[Soper, Spannowsky, PRD 2011]
χ({p, t}N) =P ({p, t}N |S)
P ({p, t}N |B)
[Buckley, Callea, Larkoski, Marzani, SciPost 2020]
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|MB|2
|MS |2'
1� cos θak + 1� cos θbk1� cos θab
,
O < 1
O > 1
Omin =1
2
××
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13Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Identifying Novel Jet ObservablesWhen likelihood ratio is not a function of standard high-level observables
Maximize
Decision
Ordering
BBN
Signal/Background Pairs
Same
Decision
Ordering?… …
…
… …
No
Yes
BBN
HLN
HL
HL
HL
HLN’
Black-Box
Guided
Search
[Faucett, JDT, Whiteson, PRD 2021; using Komiske, Metodiev, JDT, JHEP 2018]
Iteration (n) EFP κ β Chrom #
0 Mjet + pT – – –
1 2 1
22
2 0 2 2
3 0 – 1
A glimpse at an alternative history for field of jet substructure
14Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Theory-Inspired Likelihood ParametrizationsFlexible frameworks for parton-shower-like modeling
JUNIPR DGLAP White Box Ginkgo
These methods are based on constrained generative models,hopefully generalizing better than generic methods
[Andreassen, Feige, Frye, Schwartz, EPJC 2019]
−2.9
−2.4
−3.4
−3.3
−3.0 −3.0
−2.4−3.6
−2.0 −2.9
−2.4−3.2
−2.7
−3.2
−2.9
−2.9 −2.6 −2.8
Pend · Pmother · Pbranch
Pt=18 = (10−0.7)(10−0.1)(10−2.0)
[Lai, Neill, Płoskoń, Ringer, arXiv 2020] [Cranmer, Drnevich, Macaluso, Pappadopulo, arXiv 2021]
Exhibit close relationship between generation and inference
15Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Sidestepping Per-Event Likelihood Ratios?Could be helpful, though per-event information is usually complete
…therefore, (parametrized)per-event binary classifiers
can be used to constructasymptotically optimal
per-ensemble inference tools
[Nachman, JDT, arXiv 2021; see mixed sample discussion in Metodiev, Nachman, JDT, JHEP 2017]
Collider events are independent and identically distributed…
Ÿ
=1
p(xi|θA)
p(xi|θB)
p({x1, . . . , xN }|θA)
p({x1, . . . , xN }|θB)=
)
)==
NŸ
i=1
16Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
When striving for “interpretable machine learning”we are essentially hoping that likelihood ratios can beapproximated via theoretically well-motivated forms
We can impose theoretical priors by judicious choice ofnetwork architecture that captures the underlying
structures and symmetries of our problem
Machine learning methods can only be as robust and reliableas the data samples used for training
We are making progress towards uncertainty quantification,using more elaborate loss functions and training paradigms
17Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Jet Representations
[review in Kagan, arXiv 2020]
Pixelized Image
Calorimetry
… …
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Hierarchical Tree
Binary Splittings
Graphs
[e.g. Brehmer, Macaluso, Pappadopulo,Cranmer, NeurIPS 2020]
Pairwise Interactions
[e.g. Moreno, Cerri, Duarte, Newman, Nguyen,Periwal, Pierini, Serikova, Spiropulu, Vlimant, EPJC 2020]
O3
O1 O2E1
E2 E3
E4
E5 E6
Imposes implicit theoretical prior (typically a good thing!)Influences choice of network architecture
2 0 4 0 6 0 8 1 0
18Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
From Principles to Network Architectures
Permutation Equivariance Lorentz Equivariance
Infrared and Collinear SafetyLund Plane Emissions
[Dreyer, Qu, JHEP 2021]
Φ1
Φ`
100 100
y
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~Φ(p1)
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~E1
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[Dolan, Ore, PRD 2021] [Bogatskiy, Anderson, Offermann, Roussi, Miller, Kondor, arXiv 2020]
:M
k,n
T (k,n) ! T (k1,n1) ⌦ T (k2,n2),
[Komiske, Metodiev, JDT, JHEP 2019]
…
19Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Energy Flow NetworksArchitecture designed around symmetries and interpretability
[Komiske, Metodiev, JDT, JHEP 2019; see also Komiske, Metodiev, JDT, JHEP 2018; code at energyflow.network; special case of Zaheer, Kottur, Ravanbakhsh, Poczos, Salakhutdinov, Smola, NIPS 2017;
histogram pooling in Cranmer, Kreisch, Pisani, Villaescusa-Navarro, Spergel, Ho, ICLR SimDL 2021]
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V1, V2, . . . , V`
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Va
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=X
i∈J
Ei Φa(ni)
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Linear weights(IRC safe)
PermutationinvariantLatent space of dim 𝓁
Easy to plot!E
2 0 4 0 6 0 8 1 0
Learned 𝓁 = 256 latent space for quark/gluon discrimination:
20Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Learning from the Machine vs.
q g
−R −R/2 0 R/2 R
Translated Rapidity y
R
R/2
0
−R/2
−R
TranslatedAzimuthalAngle
φ
Filter 1
0.0
0.2
0.4
0.6
0.8
1.0
−R −R/2 0 R/2 R
Translated Rapidity y
R
R/2
0
−R/2
−R
TranslatedAzimuthalAngle
φ
Filter 2
0.0
0.2
0.4
0.6
0.8
1.0
0 R/8 R/4 3R/8 R/2
Radial Position θ
0.0
0.2
0.4
0.6
0.8
1.0
Rad
ialProfile
Φ(θ)
EFN2: Quark vs. Gluon
Pythia 8.230,√s = 14 TeV
R = 0.4, pT ∈ [500, 550] GeV
Learned Filter Φ1(θ)
Learned Filter Φ2(θ)
Closed-Form Φ(θ)
[Komiske, Metodiev, JDT, JHEP 2019;cf. Larkoski, JDT, Waalewijn, JHEP 2014; using Berger, Kucs, Sterman, PRD 2003; Ellis,Vermilion,Walsh, Hornig, Lee, JHEP 2010]
cf. Angularities: f(θ) = θβFor 𝓁 = 2, EFN learns radial moments: X
i∈jet
zif(θi)
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Traditional QCD observables emphasize homogeneous angular scalingBut EFN reveals that likelihood ratio exhibits collinear/wide-angle separation
21Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Learning from the Machine vs.
q g
[Komiske, Metodiev, JDT, JHEP 2019;cf. Larkoski, JDT, Waalewijn, JHEP 2014; using Berger, Kucs, Sterman, PRD 2003; Ellis,Vermilion,Walsh, Hornig, Lee, JHEP 2010]
cf. Angularities: f(θ) = θβFor 𝓁 = 2, EFN learns radial moments: X
i∈jet
zif(θi)
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EFN outperformed a domain expert (i.e. me)
But we reverse engineered the machine (and learned something about QCD)
0.0 0.2 0.4 0.6 0.8 1.0
Quark Jet Efficiency
0.0
0.2
0.4
0.6
0.8
1.0
Gluon
Jet
Rejection
EFN2: Quark vs. Gluon
Pythia 8.230,√s = 14 TeV
R = 0.4, pT ∈ [500, 550] GeV
EFN2
C(A,B)
BDT(λ(1), λ(2), λ(1/2))
Angularity λ(1)
Angularity λ(2)
Angularity λ(1/2)
Bette
r
22Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
More Network Architectures for InterpretabilityRendering the black box more transparent
[Agarwal, Hay, Iashvili, Mannix, McLean, Morris, Rappoccio, Schubert, JHEP 2021] [Kasieczka, Marzani, Soyez, Stagnitto, JHEP 2020]
Input Feature Relevance Analytic Calculations
Imposing specific theoretical structures might reduce performancebut might also yield better robustness/generalizability
23Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
When striving for “interpretable machine learning”we are essentially hoping that likelihood ratios can beapproximated via theoretically well-motivated forms
We can impose theoretical priors by judicious choice ofnetwork architecture that captures the underlying
structures and symmetries of our problem
Machine learning methods can only be as robust and reliableas the data samples used for training
We are making progress towards uncertainty quantification,using more elaborate loss functions and training paradigms
24Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Classifier1 0
Signal Background
Quark/Gluon Classification“Hello, World!” of Jet Physics
[see e.g. Gras, Höche, Kar, Larkoski, Lönnblad, Plätzer, Siódmok, Skands, Soyez, JDT, JHEP 2017;Komiske, Metodiev, Schwartz, JHEP 2017; Komiske, Metodiev, JDT, JHEP 2018]
vs.Quark
Cq = 4/3Gluon
Cg = 3 = 9/3
Find such thatQuark
Gluon
h
!
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−1
(Neyman-Pearson lemma)
Best you can do:
Likelihood ratio yields optimal binary classifier (and vice versa)
25Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Classifier1 0
Signal Background
Quark/Gluon Classification“Hello, World!” of Jet Physics
[see e.g. Gras, Höche, Kar, Larkoski, Lönnblad, Plätzer, Siódmok, Skands, Soyez, JDT, JHEP 2017;Komiske, Metodiev, Schwartz, JHEP 2017; Komiske, Metodiev, JDT, JHEP 2018]
vs.Quark
Cq = 4/3Gluon
Cg = 3 = 9/3
Likelihood ratio yields optimal binary classifier (and vice versa)
What do you mean by “quark” and “gluon”?
Jets are clusters of colorless hadrons!
Parton shower “truth” is but a (useful) fiction!
26Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
[Komiske, Metodiev, JDT, JHEP 2018; cf. ATLAS, PRD 2019; using Metodiev, Nachman, JDT, JHEP 2017; Metodiev, JDT, PRL 2018]see also Blanchard, Flaska, Handy, Pozzi, Scott, PLMR 2013; Katz-Samuels, Blanchard, Scott, JMLR 2016]
Topic Modeling to Disentangle Data Samples
0.0 2.5 5.0 7.5 10.0 12.5 15.0
Soft Drop Multiplicity nSD
0.00
0.05
0.10
0.15
0.20
ProbabilityDensity
EFP-Extracted Fractions
Pythia 8.230,√s = 14 TeV
R = 0.4, pT ∈ [500, 550] GeV
Z+jet
Dijets
Quark
Gluon
Topic 1
Topic 2
While you can’t unambiguously label individual jets, you canextract quark and gluon distributions from hadron-level measurements
Key concept from natural languageprocessing: “anchor words”
27Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Parameterized Data SamplesIncorporating nuisance parameters into training
Regardless of the approach, inspires renewed theoretical focuson uncertainty modeling for Monte Carlo generation
Learn to Pivot… …or Learn to Profile?
[Louppe, Kagan, Cranmer, NeurIPS 2017] [Ghosh, Nachman, Whiteson, arXiv 2021]
28Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
When striving for “interpretable machine learning”we are essentially hoping that likelihood ratios can beapproximated via theoretically well-motivated forms
We can impose theoretical priors by judicious choice ofnetwork architecture that captures the underlying
structures and symmetries of our problem
Machine learning methods can only be as robust and reliableas the data samples used for training
We are making progress towards uncertainty quantification,using more elaborate loss functions and training paradigms
29Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Loss Function for Bayesian AnalysesTreating network parameters as having a prior distribution
Jet Energy Scale Event Generation
Use ELBO loss to capture both statistical and systematic uncertaintiesWorth developing a frequentist version of this approach?
[Kasieczka, Luchmann, Otterpohl, Plehn, SciPost 2020] [Bellagente, Haußmann, Luchmann, Plehn, arXiv 2021]
0.0
0.2
0.4
0.6
0.8
1.0
Normalized
×10−1
BINN
Training Data
+/- σpred
20 40 60
pT,e+ [GeV]
0.9
1.0
1.1
BINN
Data
Use ELBO loss to capture both statistical and systematic uncertaintiesWorth developing a frequentist version of this approach?
Loss Function for Bayesian AnalysesTreating network parameters as having a prior distribution
30Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
<latexit sha1_base64="KEZ3fh6QsVmMKwLSft3M13nD0VI=">AAACW3icbZBNb9NAEIYnLh8lFBq+TlwWIqRWQpGNQHBBiuDCsUikrRSHaLweN6vurq3dMWpk8u/4Exy4cuAKP4C1EwFtGWmlR++8o5l9s0orz3H8tRdtXbl67fr2jf7NnVu3dwd37h76snaSJrLUpTvO0JNWliasWNNx5QhNpukoO33b9o8+kfOqtB94WdHM4IlVhZLIQZoPPqbKskgfiTzlBTGK9Kn4S9Xehj8Hkc64yZFxtS9SW/JrkRo8m28MrfOPobO38v58MIxHcVfiMiQbGI7vQ1cH88H3NC9lbciy1Oj9NIkrnjXoWElNq35ae6pQnuIJTQNaNORnTZfDSjwJSi6K0oUXftWp/040aLxfmiw4DfLCX+y14v9605qLV7NG2apmsnK9qKi14FK0oYpcOZKslwFQOhVuFXKBDiWH6M9tKWhpTbXqh2CSizFchsNno+TFKH7/fDh+s04ItuEhPIY9SOAljOEdHMAEJHyBH/ATfvW+RVtRP9pZW6PeZuYenKvowW9IdLZu</latexit>Zdθ θ p(θ|data) 6= max
θ
p(data|θ)
Nothing intrinsically wrong with Bayesian analyses,but have to be aware of cases with strong prior dependence
If needed, can treat neural networks as static objectsand calibrate them as if they were ordinary observables
[see further discussion in Cranmer, Pavez, Louppe, arXiv 2015; Nachman, SciPost 2020]
31Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Training Paradigm for Preserved Uncertainties When the goal is to maintain statistical properties
[Nachman, JDT, PRD 2020; building on Andersen, Gutschow, Maier, Prestel, EPJC 2020]
Classifier
1 0
Sample with wrong physics but all positive weights
Sample with correct physics but some negative weights
<latexit sha1_base64="dxaYhJyRgnmGu1Ql0Qq0LPx8Mz4=">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</latexit>
× w(x)⇒
<latexit sha1_base64="dxaYhJyRgnmGu1Ql0Qq0LPx8Mz4=">AAACqnicbVHbatwwEJXdW7q9bZu+9UV0KaQQFsnr+vJQWJKXPqalm6TYZpG18kZElo0kN12MP6kf1B/od1T2JtBsMiA4nJkzZ2aU14Jrg9Afx33w8NHjJ3tPR8+ev3j5avz6zamuGkXZglaiUuc50UxwyRaGG8HOa8VImQt2ll8e9/mzn0xpXsnvZlOzrCRryQtOibHUcvy7TYcmiVrnWYumcRR4fnCIpgiF2MM98EJ/5nf1sk1VCa9UJdfdwa+PHYSp4SXTcKcDGsIKfRzNgtACD6M4mHVXg+rzPfUYD0YIh0EvjOPIw9GNI62UYtQMnsvx5MYA3gX4Gkzmb8EQJ8vx33RV0aZk0lBBtE4wqk3WEmU4FawbpY1mNaGXZM0SCyWxC2XtMF8HP1hmBYtK2ScNHNj/FS0ptd6Uua0sibnQu7mevC+XNKaIspbLujFM0q1R0QhoKtj/EVzxfmOxsYBQxe2skF4QRaixP3nLpWAbWdbdyB4G757hLjj1pvjTFH31J/Oj7YXAHngH3oMDgEEI5uALOAELQJ19J3aOnGP30P3m/nCTbanrXGv2wa1wV/8AZLzHFg==</latexit>
pwrong(x)× w(x) = pcorrect(x)Plain reweighting yields all
positive weights with correctasymptotic probability density
Improved resampling throughauxiliary neural network yields correct statistical uncertainties
<latexit sha1_base64="rBiXLyd8ksjn3BORDdaFPN6e2PI=">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</latexit>
✓
δp
p
◆2
=
hw2i
hwi2
32Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Training Paradigm for Preserved Uncertainties When the goal is to maintain statistical properties
[Nachman, JDT, PRD 2020; building on Andersen, Gutschow, Maier, Prestel, EPJC 2020]
Improved resampling throughauxiliary neural network yields correct statistical uncertainties
<latexit sha1_base64="rBiXLyd8ksjn3BORDdaFPN6e2PI=">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</latexit>
✓
δp
p
◆2
=
hw2i
hwi2
Case Study in Jet Physics at Large Hadron Collider
Original sample: large weight cancellations
Reweighting recovers desired distribution
Resampling recoversdesired uncertainties
33Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
When striving for “interpretable machine learning”we are essentially hoping that likelihood ratios can beapproximated via theoretically well-motivated forms
We can impose theoretical priors by judicious choice ofnetwork architecture that captures the underlying
structures and symmetries of our problem
Machine learning methods can only be as robust and reliableas the data samples used for training
We are making progress towards uncertainty quantification,using more elaborate loss functions and training paradigms
Theory Perspective on ML for Jets
Looking forward to your thoughts and discussion!
34Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Backup Slides
35Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
[from my talk at ML4Jets 2018, with apologies]
P1 P2 P5 P8 R1
Using All Five LHC Interaction Points
36Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
E.g. Quark/Gluon ClassificationIn various limits, likelihood ratio is monotonically related to…
Away from these limits, the likelihood ratio isnot typically simple, elegant, or interpretable (but we can hope!)
log1
θ
log1
z
log1
z
log1
θ
Aemit
softdrop
, slope =
β
soft
collinear
angularcut
0 1 2 3 4 5
N
0.0
0.1
0.2
0.3
0.4
0.5
Quark
vs.
GluonAUC
Multiplicity
N-subjettiness: τ(β)N
Pythia 8.226,√s = 14 TeV
R = 0.4, pT ∈ [1000, 1100] GeV
β = 0.5
β = 1.0
β = 2.0
Soft-dropped Multiplicity IRC Safe Multiplicity
[Frye, Larkoski, JDT, Zhou, JHEP 2017] [Larkoski, Metodiev, JHEP 2019]
37Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
E.g. Detector Unfolding
Simulation
Syn
theti
cN
atu
ral
Detector-level
Data
Particle-level
Generation
Truth
Pull Weights
Push Weights
Step 1: Reweight Sim. to Data
Step 2: Reweight Gen.
νn−1
ωn
−−→ νn<latexit sha1_base64="USI/aHUkKNmen4gwHqyTXZ7rTGs=">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</latexit><latexit sha1_base64="USI/aHUkKNmen4gwHqyTXZ7rTGs=">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</latexit><latexit sha1_base64="USI/aHUkKNmen4gwHqyTXZ7rTGs=">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</latexit><latexit sha1_base64="aANR4xqa5G8N4A3PGP5I4W3UWFE=">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</latexit>
νn−1
Data−−−→ ωn
<latexit sha1_base64="IV5Rkcz2AJeiGq38yKsp/wTcRwM=">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</latexit><latexit sha1_base64="IV5Rkcz2AJeiGq38yKsp/wTcRwM=">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</latexit><latexit sha1_base64="IV5Rkcz2AJeiGq38yKsp/wTcRwM=">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</latexit><latexit sha1_base64="i+iM1Y2AuIdG+9czSK1qRLZgOsY=">AAACenicdVFNa9wwEJXdr2T7tU2OvYgshZamRq69X7dAe+gxhW4SWJtlrJW9IpJsJDnpYvRDey70V/RQ7WYLTdoOCB5v5s2bGRWN4MYS8i0I791/8PDR3n7v8ZOnz573XxycmbrVlM1oLWp9UYBhgis2s9wKdtFoBrIQ7Ly4/LDJn18xbXitvth1w3IJleIlp2A9tei7Lts2meuqyDsSjUfTOB0fkygZJkk69ICMJklKXKbaRafexQ5nXzWvVha0rq+7TEt8pwXZxvFfwH0EC87ra8kq8M2cW/QHJBqNkjSZYG9JxiSN8cZyOJ2mON4JB2gXp4v+j2xZ01YyZakAY+YxaWzegbacCuZ6WWtYA/QSKjb3UIFkJu+24zn8yjNLXNbaP2Xxlv1T0YE0Zi0LXynBrszd3Ib8V27e2nKSd1w1rWWK3hiVrcC2xpub4yXXjFqx9gCo5n5WTFeggVr/M7dcSrZWsnE9f5jf2+P/g7P3UUyi+HM6OJnsTrSHXqIj9BrFaIxO0Cd0imaIou/BfnAQHAY/w6PwTfj2pjQMdppDdCvC9Be8rLq6</latexit>
[Andreassen, Komiske, Metodiev, Nachman, JDT, PRL 2020; + Suresh, ICLR SimDL 2021;Komiske, McCormack, Nachman, arXiv 2021; see unfolding comparison in Petr Baron, arXiv 2021]
Multi-dimensional unbinned detector corrections via iterated application of likelihood ratio trick
Use ML to computereweighting factors
OmniFold
38Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
E.g. Detector Unfolding
10−5
10−4
10−3
10−2
10−1
100
Normalized
Cross
Section
Preliminary
ALEPH E.P.J. C (2004)
ALEPH Raw 1994 Data
Pythia 6 + Geant 3 Sim.
Pythia 6 Gen.
IBU ln(1− T ) + stat.
UniFold ln(1− T ) + stat.
−8 −6 −4 −2
Thrust ln(1− T )
0.85
1.0
1.15
Ratioto
Gen
.
[talk by Badea, ICHEP 2020; cf. ALEPH, EPJC 2004][see also Badea, Baty, Chang, Innocenti, Maggi, McGinn, Peters, Sheng, JDT, Lee, PRL 2019; H1, DIS2021]
Back to the Future with ALEPH Archival Data
thrust axis
intrinsicallyunbinned!
binnedarchive
[Andreassen, Komiske, Metodiev, Nachman, JDT, PRL 2020; + Suresh, ICLR SimDL 2021;Komiske, McCormack, Nachman, arXiv 2021; see unfolding comparison in Petr Baron, arXiv 2021]
39Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Energy Flow RepresentationEmphasizes infrared and collinear safety
Detection
p
p
Composite Hadrons
Quarks & Gluons
[see e.g. Sveshnikov, Tkachov, PLB 1996; Hofman, Maldacena, JHEP 2008; Mateu, Stewart, JDT, PRD 2013;Belitsky, Hohenegger, Korchemsky, Sokatchev, Zhiboedov, PRL 2014; Chen, Moult, Zhang, Zhu, PRD 2020][complementary perspective on IRC unsafe information in Chakraborty, Lim, Nojiri, Takeuchi, JHEP 2020]
Theory
E
Energy Flow:E ' lim
t→∞
niT0i(t, vtn)Robust to hadronization and detector effects
Well-defined for massless gauge theories
40Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
Machine Learning Collinear QCD
2 0 4 0.6 0.8 1.0−4 −3 −2 −1 0
EFN256: Quark vs. Gluon
Pythia 8.230,√s = 14 TeV
R = 0.4, pT ∈ [500, 550] GeV
Latent Dimension 256
Filter
Best fit, slope = 1.61
0 0 2 0.4 0.6 0
Radial Distance, lnθ
R
−1 0 −4
0.4
0.6
Pixel
Size,
lnA
πR
2
−9
−8
−7
−6
−5
−4
−3
−2
−1
0
Collinear
dPi→ig '
2αs
πCi
dθ
θ
dz
z
Soft
Cq = 4/3Cg = 3 z
θ
[Komiske, Metodiev, JDT, JHEP 2019]
vs.
q g
41Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets
0.0 0.2 0.4 0.6 0.8 1.0
Azimuthal Angle ϕ
0.0
0.2
0 π/2 π 3π/2 2π
0.0
0.5
1.0
1.5
2.0
2.5
3.0
3.5Latent Dimension 256
LogRadialDistance
lnR θ
Coordinate transformation to the emission plane
[Komiske, Metodiev, JDT, JHEP 2019; see also Dreyer, Salam, Soyez, JHEP 2018]
En Route to the Lund Plane vs.
q g