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1 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

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Page 1: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

1

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

Page 2: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

[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

Page 3: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

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

Page 4: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

4Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets

Confronting the Black Box

How do we develop robust machine learning for jet analyses?

Page 5: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

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=">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</latexit><latexit sha1_base64="/BAofgnPH6B4QebhXUNq+8pNlqE=">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</latexit><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="kPIkJdH6omNFCZSl9SSaGcCTYJg=">AAAC73iclVLLahsxFNVM+kjcR5x02Y2oKaQ0MaOp68ciEJpNFl04UCcGz2A0smYiotFMJU2oGZRt8gfdhW77Sf2BfEC+oPLYgdophV64cDj3nnsuV4pyzpT2vF+Ou/bo8ZOn6xu1Z89fvNysb22fqKyQhA5IxjM5jLCinAk60ExzOswlxWnE6Wl0fjirn15QqVgmvuhpTsMUJ4LFjGBtqXH97jPch3swiFgScCwSTmHAswSWQTV7JJMoLL3mRw/12mjXa3pV7N4zJt759s7M5bKSj1eUthuhuRJ12jNlr9f1Udf0DXy/5Pt/lnsQ/cu21237rXal7iC/GuN3Wh9a5tiM6437ofAhQAvQAIvoj+u3wSQjRUqFJhwrNUJersMSS80Ip6YWFIrmmJzjhI4sFDilKiyrdQx8a5kJjDNpU2hYsX8qSpwqNU0j25lifaZWazPyb7VRoeNuWDKRF5oKMjeKCw51BmcPDSdMUqL51AJMJLO7QnKGJSbafocll5hORZqbmj0MWj3DQ3DiN5HXRMetxsGnxYnWwWvwBuwABDrgAByBPhgA4gydS+fKuXa/ut/dG/fHvNV1FppXYCncn78B94Pc0A==</latexit>

Many QCD/collider/jet problemscan be expressed in this form!

Page 6: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

[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=">AAACunicbVFdb9MwFHXC1ygwOuCNF4sKaZuqKg6lHxJIFfDAC2JIdJvURJXj3mRWHcfYDloV5V/w5/grPOGkm8Q6rmTp6NxzfL8SJbixQfDb8+/cvXf/wd7DzqPHT/afdg+enZqi1AzmrBCFPk+oAcElzC23As6VBponAs6S9ccmf/YTtOGF/G43CuKcZpKnnFHrqGX3V6eK2l8WOkviKhi8Dch0RPrBIGijf83U6eHlUY3f4yjVlFU7LqckZOsi41Hjmk4nIZnUqnHVu/LpZBQOR618TMLWF46Hb4b1j1a+7Pau6+PbgFyB3uwFauNkeeDtR6uClTlIywQ1ZkECZeOKasuZgLoTlQYUZWuawcJBSXMwcdX2VOPXjlnhtNDuSYtb9l9HRXNjNnnilDm1F2Y315D/yy1Km07iiktVWpBsWygtBbYFbm6BV1wDs2LjAGWau14xu6BuvdZd7EaVFDYyV26OT+Dm0/DF1fqqQFNb6OMqojrL6WXt5s2ifoPcBsnuvm6D03BAggH5NuzNPmxXifbQS/QKHSKCxmiGPqMTNEcM/fGwd+Qd++/8xOf+eiv1vSvPc3QjfPsX+3PNaQ==</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

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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

“…”

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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”

Page 9: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

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

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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

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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

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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

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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

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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)=

)

)==

i=1

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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

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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

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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

~Φ(p1)

~Φ(pM)M

~E1

~EM

` `0

[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]

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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]

S�

J�

= F�

V1, V2, . . . , V`

<latexit sha1_base64="CLDgcpZzt8LjDFfYB3vgYAEsbYs=">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</latexit><latexit sha1_base64="CLDgcpZzt8LjDFfYB3vgYAEsbYs=">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</latexit><latexit sha1_base64="CLDgcpZzt8LjDFfYB3vgYAEsbYs=">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</latexit><latexit sha1_base64="m/9yOAvQkiM1IzQxy4IXGAhHNgk=">AAADCXiclVLdatswFJa9vy7dT7pd7kYsDFoIQfKa1L0YlA7G2FXHlrQQmyArcioqy0aSB8HoCfYCu23foHdjt3uKvcCeY7KbweKMwQ4IPs75vnOOPk5SCK4NQj88/9btO3fvbd3vbD94+Ohxd+fJROelomxMc5Grs4RoJrhkY8ONYGeFYiRLBDtNLl7X9dNPTGmey49mWbA4IwvJU06JcanZjrddRU2XqVokcYUGo/BgNEJ9NAgCfIiHDiA8DIf79oONEr7YhS0+aqK/AWyUEXNOiajeWQtr6R58Bd80PVotXgYYh2sthkEYHI7sZIZtvz3wH+zAsSMxz43+H1XEhGj+tjfr9n4T4CbAK9ADqziZdX9G85yWGZOGCqL1FKPCxBVRhlPBbCcqNSsIvSALNnVQkozpuGoWs/CFy8xhmiv3pIFN9k9FRTKtl1nimLWVul2rk3+rTUuThnHFZVEaJunNoLQU0OSwPgE454pRI5YOEKq42xXSc6IINe5Q1qakbCmzwnacMbhtwyaYBAOMBvj9fu/oeGXRFngGnoNdgMEBOAJvwQkYA+op74t36V35n/1r/6v/7YbqeyvNU7AW/vdfk3binQ==</latexit>

Va

J�

=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:

Page 20: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

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

Page 21: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

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

Page 22: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

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

Page 23: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

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

Page 24: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

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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h�

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−1

(Neyman-Pearson lemma)

Best you can do:

Likelihood ratio yields optimal binary classifier (and vice versa)

Page 25: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

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!

Page 26: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

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”

Page 27: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

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]

Page 28: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

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

Page 29: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

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

Page 30: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

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

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θ

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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]

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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=">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</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

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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

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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!

Page 34: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

34Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets

Backup Slides

Page 35: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

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

Page 36: Theory Perspective on Machine Learning for Jets · 2021. 6. 3. · Jesse Thaler (MIT) — Theory Perspective on Machine Learning for Jets 3 Machine learning that incorporates first

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]

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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=">AAACJ3icdVDdShtBGP1W+6Npral615vBUCgFl10bkngX6I2XFhoVsiHMTr5NBudnmZltG5Z9B1/DF/DWvoF3opfe+BydbFqo0h4YOJxzPr75TpoLbl0U3QUrq8+ev3i5tt549XrjzWbz7dax1YVhOGBaaHOaUouCKxw47gSe5gapTAWepGefF/7JNzSWa/XVzXMcSTpVPOOMOi+Nmx8TVYxLtRdXJPlh+HTmqDH6e5loiVPqncobdaQaN1tRuN/51I07JArb7YO40/Wk24kO2j0Sh1GNVn8HahyNmw/JRLNConJMUGuHcZS7UUmN40xg1UgKizllZ3SKQ08VlWhHZX1TRd57ZUIybfxTjtTq3xMlldbOZeqTkrqZfeotxH95w8JlvVHJVV44VGy5KCsEcZosCiITbpA5MfeEMsP9XwmbUUOZ8zU+2pLhXMm8avhi/lxP/k+O98M4CuMv7Va/t2wI1uAd7MIHiKELfTiEIxgAg3O4hCv4GVwE18FNcLuMrgS/Z7bhEYL7X/gNqFY=</latexit><latexit sha1_base64="aANR4xqa5G8N4A3PGP5I4W3UWFE=">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</latexit>

νn−1

Data−−−→ ωn

<latexit sha1_base64="IV5Rkcz2AJeiGq38yKsp/wTcRwM=">AAACenicdVFLa9wwEJbdV7J9ZJP01ovIUmhpauTa+7ottIceU+gmgbVZZK3sFdHDSHLaxeiH9lzor+ihWm8KTdoOCD6+mW++mVFRc2YsQt+C8N79Bw8f7e33Hj95+uygf3h0blSjCZ0TxZW+LLChnEk6t8xyellrikXB6UVx9X6bv7im2jAlP9tNTXOBK8lKRrD11LLv2qxrstBVkbcoGo+mcTo+RVEyTJJ06AEaTZIUuUw2y1a+jR3MvmpWrS3WWn1pMy3gnRaoi9O/gPuALXZerwStsG/m3LI/QNFolKTJBHpLNEZpDLeWw+k0hfGNcDB7Dro4W/Z/ZCtFGkGlJRwbs4hRbfMWa8sIp66XNYbWmFzhii48lFhQk7fdeA6+9MwKlkr7Jy3s2D8VLRbGbEThKwW2a3M3tyX/lVs0tpzkLZN1Y6kkO6Oy4dAquL05XDFNieUbDzDRzM8KyRprTKz/mVsuJd1IUbueP8zv7eH/wfm7KEZR/CkdzCa7C4E98AKcgFcgBmMwAx/BGZgDAr4H+8FRcBz8DE/C1+GbXWkY3GiOwa0I0181Z7sO</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=">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</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

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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]

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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

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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

θ

dz

z

Soft

Cq = 4/3Cg = 3 z

θ

[Komiske, Metodiev, JDT, JHEP 2019]

vs.

q g

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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