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Paper Citation Record · LEDGER

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV

As of 13 August 2026, this Paper Citation Record lists 100 of 122 outbound references and 1 inbound Pith citation observation for arXiv:2411.16907.

A citation records a reference. It does not transfer a finding from one paper to another.

pith.paper-citation-record.v1
2411.16907 v2

Coverage vector

measured 100 of 122 reference resolution

Typed states for the displayed outbound observations.

Source: paper_references, paper_reference_links, observed 2026-08-12T12:51:25.728284Z

measured 101 of 101 standing notices

One-hop event checks from named stored sources.

Source: scholarly_work_events, retraction_status_cache, observed 2026-08-12T06:34:41.77262+00:00

measured 1 of 1 inbound itemization

Pith citing papers itemized under the disclosed page cap.

Source: paper_references, paper_reference_links, observed 2026-08-12T04:24:21.013722Z

measured 0 of 1 external citation measurements

A source-named dated measurement, never combined with another source.

Source: pith, observed 2026-08-12T04:24:23.020238Z

Reference resolution

100 of 122 outbound references displayed

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  • verified fuzzy0
  • unresolved94
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External citation measurements

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Outbound references

Observation 24648bce-8df7-4fdb-99f6-219f268ce1d4 · outbound

This paper cites Broken symmetry and the mass of gauge vector mesons.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV Broken symmetry and the mass of gauge vector mesons

Reference 1

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source=pdf_text observed=2026-08-12T12:51:25.325321Z digest=sha256:ace6a0c99c71582c10fb481aea3993b015d3f9207353a99e1563e2f38c6b76f0

Observation 317db6d4-3f1c-4d7b-aa9c-eb1c4c4ddab4 · outbound

This paper cites Broken symmetries, massless particles and gauge fields.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV Broken symmetries, massless particles and gauge fields

Reference 2

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source=pdf_text observed=2026-08-12T12:51:25.330084Z digest=sha256:c629e949930b4de85d5382720f7d26db7b2e2293e42a69878289d9da1d99abe6

Observation 5dd8c231-9c5f-4c8c-bcc1-118ba883c304 · outbound

This paper cites Broken symmetries and the masses of gauge bosons.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV Broken symmetries and the masses of gauge bosons

Reference 3

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source=pdf_text observed=2026-08-12T12:51:25.334302Z digest=sha256:fe5426a9e9f8b5138524ad4f7f7c3283cbfc1be9fca6aa20e33e3e018901cafa

Observation 7e2d3906-0418-4388-8c41-931659ea8da1 · outbound

This paper cites Global conservation laws and massless particles.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV Global conservation laws and massless particles

Reference 4

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source=pdf_text observed=2026-08-12T12:51:25.338325Z digest=sha256:1d95d21ec7adc5e35b0975341fe0d1693df65375f9223de8346c2ea8f97c88f8

Reference 5

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source=pdf_text observed=2026-08-12T12:51:25.342446Z digest=sha256:3e32c1de303deae793b309652c4d9e1cfe760576217357051f7aafba77ec9e02

Reference 6

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source=pdf_text observed=2026-08-12T12:51:25.346803Z digest=sha256:ccf16176bbac1b11484215ec2b226f09a1a756411b15f7a556a89e3534858db5

Reference 7

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source=pdf_text observed=2026-08-12T12:51:25.351699Z digest=sha256:7af3b4b4ef48f32ecb27825a69192d0ab12f5f5a70a85e0621010e2a7f259b70

Reference 8

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Reference 9

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source=pdf_text observed=2026-08-12T12:51:25.360129Z digest=sha256:84f70324556dc9d1b38039132737c775ea770ee6587f1ae771d6b906b34282ac

Observation abcd211c-9842-498d-82eb-ced80dfae625 · outbound

This paper cites Measurements of $WH$ and $ZH$ production with Higgs boson decays into bottom quarks and direct constraints on the charm Yukawa coupling in $13\,\mathrm{TeV}$ $pp$ collisions with the ATLAS detector.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV Measurements of $WH$ and $ZH$ production with Higgs boson decays into bottom quarks and direct constraints on the charm Yukawa coupling in $13\,\mathrm{TeV}$ $pp$ collisions with the ATLAS detector

Reference 10

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source=pdf_text observed=2026-08-12T12:51:25.364075Z digest=sha256:0df755ab5967df21d823b9ca2594bc91aa9610a03bb400aaec3a86c49da212b4

Observation 4c211a24-79f9-41dc-8a43-f3a4f6513f1a · outbound

This paper cites Measurement of simplified template cross sections of the Higgs boson produced in association with W or Z bosons in the H $\to$ $\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV Measurement of simplified template cross sections of the Higgs boson produced in association with W or Z bosons in the H $\to$ $\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV

Reference 11

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source=pdf_text observed=2026-08-12T12:51:25.368246Z digest=sha256:b667fd923416c32694cef1e07e6e28e08136e7a3fca1d2c8defde024793f2fa2

Observation 622b0dc2-ca31-4cc0-8e8c-4388d312fda2 · outbound

This paper cites Effective Lagrangian analysis of new interactions and flavor conservation.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV Effective Lagrangian analysis of new interactions and flavor conservation

Reference 12

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source=pdf_text observed=2026-08-12T12:51:25.372106Z digest=sha256:6bfb490684663f0dd8c4bbeee5f14284b48536cf16aef9607ac02d1eaaab68eb

Observation 60fffde3-e7e2-428d-b758-8860b90ecfd4 · outbound

This paper cites Operator analysis for precision electroweak physics.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV Operator analysis for precision electroweak physics

Reference 13

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doi, observed 2026-08-12T12:51:25.933334Z

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No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

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Reference 14

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source=pdf_text observed=2026-08-12T12:51:25.379913Z digest=sha256:b179b191fc9cf6164492c3e0c380ad1ae4cfac5d8cd62d8d342e7fd40f240b79

Reference 15

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Reference 16

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Reference 17

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Reference 18

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Reference 19

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Reference 20

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Reference 21

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Reference 22

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Reference 24

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Reference 29

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source=pdf_text observed=2026-08-12T12:51:25.440560Z digest=sha256:8144f1d52ce2e56a3986c5220fb047605d7b54882194a97a8a1d6ac71198cba6

Observation 7f2f8e00-9b02-45d7-b882-def67ed5a6bd · outbound

This paper cites Combined Higgs boson production and decay measurements with up to 137 fb−1 of proton-proton collision data at √s = 13 TeV.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV Combined Higgs boson production and decay measurements with up to 137 fb−1 of proton-proton collision data at √s = 13 TeV

Reference 30

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source=pdf_text observed=2026-08-12T12:51:25.444503Z digest=sha256:7322fabb91c47357fd1dfcb055a71a43683aa87451cb5af4dab9ee3c7162e980

Reference 31

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source=pdf_text observed=2026-08-12T12:51:25.448404Z digest=sha256:7bb5a6b60b3853990d9196b9570cbb167c8ff70defc549ef04b29d5a18ebc370

Reference 32

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source=pdf_text observed=2026-08-12T12:51:25.452454Z digest=sha256:b71e5ca98bf79ebf7439a87f6017a3a12ac81845d9aa5707fd66c5ed582788b5

Observation d8ce29d3-ab69-4a8e-93fd-ea6acfc08e01 · outbound

This paper cites HEPData record for this analysis.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV HEPData record for this analysis

Reference 33

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No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T12:51:25.456489Z digest=sha256:901c2fd258cd1d34892052b6bad474efe317533aa80e9d170baad2356f6f6b0e

Observation 43242ae6-ebbd-4747-9f02-28d9b07ac11e · outbound

This paper cites Baryon- and lepton-nonconserving processes.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV Baryon- and lepton-nonconserving processes

Reference 34

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Reference 35

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Reference 36

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Reference 37

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Reference 38

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Reference 39

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Reference 40

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Reference 41

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source=pdf_text observed=2026-08-12T12:51:25.488203Z digest=sha256:004099e9c1108b2f9a91a403adf1f1c72139271b759543a2cb23222d05cc82a8

Observation a3c511ac-2364-4865-9013-762be87e7c6f · outbound

This paper cites Tree boosting for learning EFT parameters.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV Tree boosting for learning EFT parameters

Reference 42

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source=pdf_text observed=2026-08-12T12:51:25.492236Z digest=sha256:6be8ecad8771fe7a5c57ceae5e469718393ca4270d3e2cf9cfc241068fa53a62

Reference 43

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source=pdf_text observed=2026-08-12T12:51:25.496017Z digest=sha256:dd480a695cad09d10229608d01a0ae410eacc7f0ac63fa9a566f50b9fd3d836d

Reference 44

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Reference 45

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source=pdf_text observed=2026-08-12T12:51:25.504136Z digest=sha256:9a946de7b7f681ece14fbb3105e1ff8f675e862096b854a86815a2ffa316e535

Reference 46

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local_arxiv, observed 2026-08-12T12:51:26.814410Z

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No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

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Reference 47

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source=pdf_text observed=2026-08-12T12:51:25.512564Z digest=sha256:97bd5f7328edabeb431a567f2034d90ac54d664e31103fcbe15f6c01c2e16705

Observation 57ba8af4-14e5-459b-8492-118010a47b92 · outbound

This paper cites The CMS experiment at the CERN LHC.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV The CMS experiment at the CERN LHC

Reference 48

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source=pdf_text observed=2026-08-12T12:51:25.516862Z digest=sha256:41e141fb187ac341a92ec8bc07724cdcd0a1125fd7a98c59e42a223e36cb6ab2

Reference 49

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source=pdf_text observed=2026-08-12T12:51:25.520886Z digest=sha256:67287c014ca8a2af3f6df7b54b6ebedba99be5d95bae2652cecd144a57d35830

Reference 50

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source=pdf_text observed=2026-08-12T12:51:25.524892Z digest=sha256:f0a2e9027b8783e16a038a40720458f623a877f91baa5521973697898f052d77

Reference 51

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source=pdf_text observed=2026-08-12T12:51:25.528881Z digest=sha256:af645d92b403a452a334298f591a6866e2cc999cb546ed37913d8f834fd7370a

Observation cc5ea783-06ea-44c2-8830-fbe13274cba5 · outbound

This paper cites Track impact parameter resolution for the full pseudo rapidity coverage in the 2017 dataset with the CMS phase-1 pixel detector.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV Track impact parameter resolution for the full pseudo rapidity coverage in the 2017 dataset with the CMS phase-1 pixel detector

Reference 52

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source=pdf_text observed=2026-08-12T12:51:25.532851Z digest=sha256:6ded8e8ad4602bfa3b6f90f6751f7fe045242bd38119b04e755249f4fa92d41f

Reference 53

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source=pdf_text observed=2026-08-12T12:51:25.536664Z digest=sha256:5015fd435f6c735ce33963831ca8f907ec6afd79b4762b334dfb09a7d28ec2e3

Reference 54

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source=pdf_text observed=2026-08-12T12:51:25.540576Z digest=sha256:deaa4942a5f23e85a7e0e05c391abef4ed8c294119ddeae7e2b4a5d270ea376b

Reference 55

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source=pdf_text observed=2026-08-12T12:51:25.544910Z digest=sha256:196a08190a915894a29bbf88e8db2bc5cf50e11d0fffd6f5c509419e1c14750e

Reference 56

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verified exact
local_arxiv, observed 2026-08-12T12:51:26.701944Z

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source=pdf_text observed=2026-08-12T12:51:25.548927Z digest=sha256:84403afc03f184e119e09425493c4d5b83c2dff8ee806e18ffc537f43bb35295

Reference 57

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source=pdf_text observed=2026-08-12T12:51:25.552952Z digest=sha256:1c3351dd78c18ede1c7175e23303c37a972dad59772b0ba076846ba82a634bcc

Reference 58

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source=pdf_text observed=2026-08-12T12:51:25.556941Z digest=sha256:fbac2646f4280b984c3710e05113a4741ffe2321b58ef84b2c04e21306309afd

Reference 59

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source=pdf_text observed=2026-08-12T12:51:25.560840Z digest=sha256:add858c8865749f65b7931f2986b4fbba58295344688ca573d1e3562fd521a64

Reference 60

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source=pdf_text observed=2026-08-12T12:51:25.564924Z digest=sha256:d23ed9d9b1e7b20fda2cc7c060d375ef155e810b89ca1dcd5633426671beacd9

Reference 61

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source=pdf_text observed=2026-08-12T12:51:25.568891Z digest=sha256:3b16c4c98a7f1d6aaf0cc24e2443aaf517a3bfb837a6b3fe75aeb0f586a81c06

Reference 62

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source=pdf_text observed=2026-08-12T12:51:25.572786Z digest=sha256:5de75dced6caaec0900a46d68320d4e1a919d07851a41c7c88f83b4dbd285c11

Reference 63

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source=pdf_text observed=2026-08-12T12:51:25.577001Z digest=sha256:51eadbf11191635fb0bf49f3586c4dd59829ce3769287fc3a11c0c2b3436350d

Reference 64

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source=pdf_text observed=2026-08-12T12:51:25.581010Z digest=sha256:2a0ebadfa87e185410b42d0113499bea81dd7d3e639d90cd829fc896e162d672

Reference 65

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source=pdf_text observed=2026-08-12T12:51:25.585050Z digest=sha256:0123d220de36e8a18088b1c30ef9e10be87b4d28c0dd86ae04c65189a04c016c

Reference 66

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source=pdf_text observed=2026-08-12T12:51:25.589090Z digest=sha256:631c0f6a433a75b10e5e8b4ca396547f2bb81abecc65445e92cf35ec1c5815ef

Reference 67

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source=pdf_text observed=2026-08-12T12:51:25.592896Z digest=sha256:fb7842950de4bf1f38844ae38c438785fce6ceac87bbbe4916ec4bb4826a966f

Reference 68

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verified exact
local_arxiv, observed 2026-08-12T12:51:26.547095Z

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source=pdf_text observed=2026-08-12T12:51:25.597145Z digest=sha256:0ad984d927c0adf40b7a59eb85ae5117c03d40b1028e4fabc817ae1e4110c86a

Reference 69

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source=pdf_text observed=2026-08-12T12:51:25.601225Z digest=sha256:43637ceaa89e08ad3e7f8d3997e4bccb33492f3656e03f51a2489b9301459326

Reference 70

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source=pdf_text observed=2026-08-12T12:51:25.605196Z digest=sha256:f638ba1efc1c0dec8327acfc810f24347e8c155cc894ea0c3575d528bb6a4fc4

Reference 71

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source=pdf_text observed=2026-08-12T12:51:25.609576Z digest=sha256:440fd24224e17df3751c438b5b06f0580173d6487edcf1e54127062fcedb06c8

Reference 72

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source=pdf_text observed=2026-08-12T12:51:25.613632Z digest=sha256:770e5c8e75f8e39cf7d5c9bfafb4dd190bc7262fcc1ec528f98ea11eb4c6e6ca

Reference 73

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source=pdf_text observed=2026-08-12T12:51:25.617636Z digest=sha256:35d5db1e22f6d765a6b6e496fbe39555dff3ae41d02f978ff5f79dc3c04d03db

Observation 2eebce88-4fd3-4068-a310-06f3985c978c · outbound

This paper cites MadWeight: automatic event reweighting with matrix elements.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV MadWeight: automatic event reweighting with matrix elements

Reference 74

Resolution
verified exact
doi, observed 2026-08-12T12:51:25.885104Z

Source-reported events for the cited work

No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T12:51:25.621740Z digest=sha256:8dfe1da08982d287eeb5bceb93b5e072028bdfee3e42db8beb76a8a2ab53b613

Reference 75

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unresolved
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source=pdf_text observed=2026-08-12T12:51:25.625572Z digest=sha256:ebf12fe54b6b3dcde0db8c2db9044a9e9c74c90a6bab5998507a8c70c4062d19

Reference 76

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source=pdf_text observed=2026-08-12T12:51:25.629437Z digest=sha256:a1c1cd5ee76cc7ed360f63254175d1e077ba1fc2d1aa6231906b2a85edb86312

Reference 77

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source=pdf_text observed=2026-08-12T12:51:25.633454Z digest=sha256:45474b16b9708d306bd57997bb1c03eff38a130bd58bd5947d05a05378db3b2d

Observation acea65bc-9bdf-4bf1-92ff-ce649f7cf7b2 · outbound

This paper cites G EANT 4—a simulation toolkit.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV G EANT 4—a simulation toolkit

Reference 78

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source=pdf_text observed=2026-08-12T12:51:25.637537Z digest=sha256:b6b4904ffa7f5ba1928b1ba28f44d9508117d7f24bb4c38cf5950c41bcf86a4b

Observation a686b3b5-4b2f-45fd-94a9-6cefe80bcb6f · outbound

This paper cites Technical proposal for the Phase-II upgrade of the Compact Muon Solenoid.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV Technical proposal for the Phase-II upgrade of the Compact Muon Solenoid

Reference 79

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source=pdf_text observed=2026-08-12T12:51:25.641675Z digest=sha256:847abc076b8f51886e11eb8a5e07aff3e23bf16e78c779b168564556d9cfbc71

Reference 80

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source=pdf_text observed=2026-08-12T12:51:25.645521Z digest=sha256:75a6aeafd9436d604a367367df7c2fc3c59fc3c27ade6b0207d1d76fdfc3e937

Observation 99622ed5-cc5e-4489-9d40-45392a132796 · outbound

This paper cites ECAL 2016 refined calibration and Run2 summary plots.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV ECAL 2016 refined calibration and Run2 summary plots

Reference 81

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source=pdf_text observed=2026-08-12T12:51:25.649762Z digest=sha256:a52cc19fd30b2825fa31c07b853e577ff68eaa83c1e869e2f1186814a67cfcc7

Reference 82

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source=pdf_text observed=2026-08-12T12:51:25.653528Z digest=sha256:cc443f1460d7987f2deca8d4f2bfc78e4ffd6321fd054e737cc643b68b25bf97

Reference 83

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source=pdf_text observed=2026-08-12T12:51:25.657701Z digest=sha256:3574fe16ca3b9e5ccf66599f209974462801f5279c5546ec925c160dd66cf1a9

Reference 84

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source=pdf_text observed=2026-08-12T12:51:25.661688Z digest=sha256:e0ee2981c5b0ea96d6cc00edf4e6256227683e5108559e0b97af73e3b2049e04

Observation 2cb95a73-5393-45d1-8c43-85962513884c · outbound

This paper cites Jet energy scale and resolution measurement with Run 2 legacy data collected by CMS at 13 TeV.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV Jet energy scale and resolution measurement with Run 2 legacy data collected by CMS at 13 TeV

Reference 85

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source=pdf_text observed=2026-08-12T12:51:25.666737Z digest=sha256:bd0fc06b181b822db4c8c5eaca85cc4461ec7e831d94a5a9dea93749952202f0

Reference 86

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source=pdf_text observed=2026-08-12T12:51:25.670534Z digest=sha256:1c2b5ee6e103fc9a6fdd37aa7a8d480be69b3bec42e886535f05bbabd387aa87

Reference 87

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source=pdf_text observed=2026-08-12T12:51:25.675658Z digest=sha256:94199ef3700f85d25ff831cc07c1a3f4104e7fa7353b2119f0dfc10db1930d1d

Reference 88

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source=pdf_text observed=2026-08-12T12:51:25.679658Z digest=sha256:741f8133fae93a985793bf9f370cffbc067507680cf38f221ee7120c0a094320

Reference 89

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source=pdf_text observed=2026-08-12T12:51:25.683547Z digest=sha256:41ea111cf182bfe17c10c2f45e79e060f61197a513cb3aabc487b4cdd9d506dc

Observation ebe8f308-9178-40c4-8905-5a1dc57f58a3 · outbound

This paper cites Jet algorithms performance in 13 TeV data.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV Jet algorithms performance in 13 TeV data

Reference 90

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source=pdf_text observed=2026-08-12T12:51:25.687673Z digest=sha256:a8c7fe4425169e38d73991c97195aefd852e56da0f8ab41b94987664701c8af1

Reference 91

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source=pdf_text observed=2026-08-12T12:51:25.691462Z digest=sha256:f98b2578bb0a3d41d7b1af6ba811cf734d00cacbba2699fb0b617f6b663e0c50

Observation 9145f5c9-c2eb-4d60-ad22-0cc1e45ae2e5 · outbound

This paper cites Performance summary of AK4 jet b tagging with data from proton-proton collisions at 13 TeV.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV Performance summary of AK4 jet b tagging with data from proton-proton collisions at 13 TeV

Reference 92

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source=pdf_text observed=2026-08-12T12:51:25.695479Z digest=sha256:9f4550dd89fd445f722acb839b9b92e34841bea3d5d6491764e26a8eeb848260

Reference 93

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source=pdf_text observed=2026-08-12T12:51:25.699319Z digest=sha256:99401aa9f420e1854f38e5afce352882dea0c78ca067bab13dcce7b3abf36494

Reference 94

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source=pdf_text observed=2026-08-12T12:51:25.703304Z digest=sha256:1b193e8ff08f60a9f344a7794e30136e0370cb5c443e3e17b0017dd93d104951

Reference 95

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source=pdf_text observed=2026-08-12T12:51:25.707877Z digest=sha256:5717fa2d3cb5d8e759ebff9b9f14417779b8e4726064a4e6d6cb892cfed3e3ef

Reference 96

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source=pdf_text observed=2026-08-12T12:51:25.712102Z digest=sha256:088520503ddd3b097a726ec0bba951d1c144b2272c408aaf797c29b963110173

Reference 97

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source=pdf_text observed=2026-08-12T12:51:25.716004Z digest=sha256:909ee8423d2827934e41532d384227854bf09cab6795b8b8b09ba553c10f0535

Reference 98

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source=pdf_text observed=2026-08-12T12:51:25.719922Z digest=sha256:24a31894874be34254c8bbc636e8876b08afcdb524f4ae370902b1608251be2c

Reference 99

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source=pdf_text observed=2026-08-12T12:51:25.724113Z digest=sha256:430a5adc50fb4f4ee5862bc5af4ea897605f20037e7f73daf60919cf14c791dd

Observation c45b26ea-a2a9-4f89-8f19-90432daf5a48 · outbound

This paper cites Identification of highly Lorentz-boosted heavy particles using graph neural networks and new mass decorrelation techniques.

Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV Identification of highly Lorentz-boosted heavy particles using graph neural networks and new mass decorrelation techniques

Reference 100

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source=pdf_text observed=2026-08-12T12:51:25.728284Z digest=sha256:3a710976ed46999a615fb1f127d0c992af9c792085f725336c685c73a96cc1d8

Pith citing papers

Observation c5c5f216-9f68-4082-a871-a09a8e0a7cfd · inbound

Measurement of off-shell Higgs boson production in the $H^*\rightarrow ZZ\rightarrow 4\ell$ decay channel using a neural simulation-based inference technique in 13 TeV $pp$ collisions with the ATLAS detector cites this paper.

Measurement of off-shell Higgs boson production in the $H^*\rightarrow ZZ\rightarrow 4\ell$ decay channel using a neural simulation-based inference technique in 13 TeV $pp$ collisions with the ATLAS detector Constraints on standard model effective field theory for a Higgs boson produced in association with W or Z bosons in the H $\to\mathrm{b\bar{b}}$ decay channel in proton-proton collisions at $\sqrt{s}$ = 13 TeV

Reference 33

Resolution
verified exact
local_arxiv, observed 2026-08-12T04:24:23.025748Z

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No event found in the named queried sources as of 2026-08-12T06:34:41.77262+00:00.

source=pdf_text observed=2026-08-12T04:24:21.013722Z digest=sha256:cafffd7c48d6993b9eb6a85c8cb9bd9678b4632fda5554a43be22964d183ff09