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Paper Citation Record · LEDGER

Improved analysis of non-resonant Higgs boson pair production in the $b\bar{b}\tau^+\tau^-$ final state with $196$ fb$^{-1}$ of data collected at $\sqrt{s}$ = 13 TeV and 13.6 TeV with the ATLAS detector

As of 18 August 2026, this Paper Citation Record lists 100 of 140 outbound references and 0 inbound Pith citation observations for arXiv:2607.26879.

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

pith.paper-citation-record.v1
2607.26879 v1

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measured 100 of 140 reference resolution

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Outbound references

Reference 1

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Reference 2

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Reference 3

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Observation 7280edf4-fc35-4027-a670-bd0b76ef9b41 · outbound

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

Improved analysis of non-resonant Higgs boson pair production in the $b\bar{b}\tau^+\tau^-$ final state with $196$ fb$^{-1}$ of data collected at $\sqrt{s}$ = 13 TeV and 13.6 TeV with the ATLAS detector Higgs,Broken symmetries, massless particles and gauge fields, Phys

Reference 4

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Reference 5

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Reference 6

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Reference 7

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Reference 8

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Reference 9

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Reference 10

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Observation 2767eea5-e735-4d4f-9b3a-79456f1f1c7c · outbound

This paper cites Combined measurement of the Higgs boson mass from the $H\to\gamma\gamma$ and $H\to ZZ^{*} \to 4\ell$ decay channels with the ATLAS detector using $\sqrt{s}$ = 7, 8 and 13 TeV $pp$ collision data.

Improved analysis of non-resonant Higgs boson pair production in the $b\bar{b}\tau^+\tau^-$ final state with $196$ fb$^{-1}$ of data collected at $\sqrt{s}$ = 13 TeV and 13.6 TeV with the ATLAS detector Combined measurement of the Higgs boson mass from the $H\to\gamma\gamma$ and $H\to ZZ^{*} \to 4\ell$ decay channels with the ATLAS detector using $\sqrt{s}$ = 7, 8 and 13 TeV $pp$ collision data

Reference 11

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Reference 12

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Observation 6ff47d9c-a3c0-4ff9-9ff3-39a313a73377 · outbound

This paper cites $CP$ Properties of Higgs Boson Interactions with Top Quarks in the $t\bar{t}H$ and $tH$ Processes Using $H \rightarrow \gamma\gamma$ with the ATLAS Detector.

Improved analysis of non-resonant Higgs boson pair production in the $b\bar{b}\tau^+\tau^-$ final state with $196$ fb$^{-1}$ of data collected at $\sqrt{s}$ = 13 TeV and 13.6 TeV with the ATLAS detector $CP$ Properties of Higgs Boson Interactions with Top Quarks in the $t\bar{t}H$ and $tH$ Processes Using $H \rightarrow \gamma\gamma$ with the ATLAS Detector

Reference 13

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Reference 14

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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 23

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Reference 24

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Reference 25

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Reference 26

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Reference 27

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Reference 28

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Reference 29

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Reference 30

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Reference 31

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Reference 32

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Reference 34

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Observation 5652c455-9474-429d-8800-469e6f244b93 · outbound

This paper cites Search for nonresonant pair production of Higgs bosons in the $b\bar{b}b\bar{b}$ final state in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector.

Improved analysis of non-resonant Higgs boson pair production in the $b\bar{b}\tau^+\tau^-$ final state with $196$ fb$^{-1}$ of data collected at $\sqrt{s}$ = 13 TeV and 13.6 TeV with the ATLAS detector Search for nonresonant pair production of Higgs bosons in the $b\bar{b}b\bar{b}$ final state in $pp$ collisions at $\sqrt{s}= 13$ TeV with the ATLAS detector

Reference 35

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Observation 59831d58-c5ec-4a0b-b739-8ce480f5c673 · outbound

This paper cites Search for pair production of boosted Higgs bosons via vector-boson fusion in the $b\bar{b}b\bar{b}$ final state using $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector.

Improved analysis of non-resonant Higgs boson pair production in the $b\bar{b}\tau^+\tau^-$ final state with $196$ fb$^{-1}$ of data collected at $\sqrt{s}$ = 13 TeV and 13.6 TeV with the ATLAS detector Search for pair production of boosted Higgs bosons via vector-boson fusion in the $b\bar{b}b\bar{b}$ final state using $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector

Reference 36

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Reference 37

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Observation 95567ec4-45bb-4f20-9868-053cd46543d0 · outbound

This paper cites Search for nonresonant Higgs boson pair production in final states with two bottom quarks and two photons in proton-proton collisions at $\sqrt{s} =$ 13 TeV.

Improved analysis of non-resonant Higgs boson pair production in the $b\bar{b}\tau^+\tau^-$ final state with $196$ fb$^{-1}$ of data collected at $\sqrt{s}$ = 13 TeV and 13.6 TeV with the ATLAS detector Search for nonresonant Higgs boson pair production in final states with two bottom quarks and two photons in proton-proton collisions at $\sqrt{s} =$ 13 TeV

Reference 38

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Observation 1702fe96-dbee-4694-a98a-807047447932 · outbound

This paper cites Studies of new Higgs boson interactions through nonresonant $HH$ production in the $b\bar{b}\gamma\gamma$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector.

Improved analysis of non-resonant Higgs boson pair production in the $b\bar{b}\tau^+\tau^-$ final state with $196$ fb$^{-1}$ of data collected at $\sqrt{s}$ = 13 TeV and 13.6 TeV with the ATLAS detector Studies of new Higgs boson interactions through nonresonant $HH$ production in the $b\bar{b}\gamma\gamma$ final state in $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector

Reference 39

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Observation c040b27e-2694-453f-9403-62d5846e70bf · outbound

This paper cites Study of Higgs boson pair production in the $HH \rightarrow b \overline{b} \gamma \gamma$ final state with 308 fb$^{-1}$ of data collected at $\sqrt{s} =$ 13 TeV and 13.6 TeV by the ATLAS experiment.

Improved analysis of non-resonant Higgs boson pair production in the $b\bar{b}\tau^+\tau^-$ final state with $196$ fb$^{-1}$ of data collected at $\sqrt{s}$ = 13 TeV and 13.6 TeV with the ATLAS detector Study of Higgs boson pair production in the $HH \rightarrow b \overline{b} \gamma \gamma$ final state with 308 fb$^{-1}$ of data collected at $\sqrt{s} =$ 13 TeV and 13.6 TeV by the ATLAS experiment

Reference 40

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Observation df96a489-bd53-43b9-9dd1-af3cb8a7394f · outbound

This paper cites Search for resonant and non-resonant Higgs boson pair production in the $b\bar b\tau^+\tau^-$ decay channel using 13 TeV $pp$ collision data from the ATLAS detector.

Improved analysis of non-resonant Higgs boson pair production in the $b\bar{b}\tau^+\tau^-$ final state with $196$ fb$^{-1}$ of data collected at $\sqrt{s}$ = 13 TeV and 13.6 TeV with the ATLAS detector Search for resonant and non-resonant Higgs boson pair production in the $b\bar b\tau^+\tau^-$ decay channel using 13 TeV $pp$ collision data from the ATLAS detector

Reference 41

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Observation 649302ab-fb63-4b46-beb6-7cbecb1ce746 · outbound

This paper cites Search for nonresonant Higgs boson pair production in final state with two bottom quarks and two tau leptons in proton-proton collisions at $\sqrt{s}$ = 13 TeV.

Improved analysis of non-resonant Higgs boson pair production in the $b\bar{b}\tau^+\tau^-$ final state with $196$ fb$^{-1}$ of data collected at $\sqrt{s}$ = 13 TeV and 13.6 TeV with the ATLAS detector Search for nonresonant Higgs boson pair production in final state with two bottom quarks and two tau leptons in proton-proton collisions at $\sqrt{s}$ = 13 TeV

Reference 42

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Observation bcd2064b-3d85-4577-b77d-d5eece17d434 · outbound

This paper cites Search for the non-resonant production of Higgs boson pairs via gluon fusion and vector-boson fusion in the $b\bar{b}\tau^+\tau^-$ final state in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector.

Improved analysis of non-resonant Higgs boson pair production in the $b\bar{b}\tau^+\tau^-$ final state with $196$ fb$^{-1}$ of data collected at $\sqrt{s}$ = 13 TeV and 13.6 TeV with the ATLAS detector Search for the non-resonant production of Higgs boson pairs via gluon fusion and vector-boson fusion in the $b\bar{b}\tau^+\tau^-$ final state in proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector

Reference 43

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Observation 659fc6fb-7402-457a-b550-56ee8c32de58 · outbound

This paper cites Search for non-resonant Higgs boson pair production in final states with leptons, taus, and photons in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector.

Improved analysis of non-resonant Higgs boson pair production in the $b\bar{b}\tau^+\tau^-$ final state with $196$ fb$^{-1}$ of data collected at $\sqrt{s}$ = 13 TeV and 13.6 TeV with the ATLAS detector Search for non-resonant Higgs boson pair production in final states with leptons, taus, and photons in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector

Reference 44

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Reference 45

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source=pdf_text observed=2026-07-30T18:22:14.501375Z digest=sha256:611ef653b169fd14d82e42f40091ab4dffc7d32e59cf4762f441458e9c7db1ad

Observation 56bcaabe-b370-4e09-acca-542dd735b708 · outbound

This paper cites Search for non-resonant Higgs boson pair production in the $2b + 2\ell + E_\mathrm{T}^\mathrm{miss}$ final state in $pp$ collisions $\sqrt{s} = 13\,\mathrm{TeV}$ with the ATLAS detector.

Improved analysis of non-resonant Higgs boson pair production in the $b\bar{b}\tau^+\tau^-$ final state with $196$ fb$^{-1}$ of data collected at $\sqrt{s}$ = 13 TeV and 13.6 TeV with the ATLAS detector Search for non-resonant Higgs boson pair production in the $2b + 2\ell + E_\mathrm{T}^\mathrm{miss}$ final state in $pp$ collisions $\sqrt{s} = 13\,\mathrm{TeV}$ with the ATLAS detector

Reference 46

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source=pdf_text observed=2026-07-30T18:22:14.562054Z digest=sha256:db2616e924ada77700c483af230bdbab6a84ab91671e3e5278bc52d24f36c065

Observation 1443ee8e-2c2f-4f72-bcdf-e8027caea6b3 · outbound

This paper cites Search for Higgs boson pair production in the $\mathrm{b}\overline{\mathrm{b}}$W$^+$W$^-$ decay mode in proton-proton collisions at $\sqrt{s}$ = 13 TeV.

Improved analysis of non-resonant Higgs boson pair production in the $b\bar{b}\tau^+\tau^-$ final state with $196$ fb$^{-1}$ of data collected at $\sqrt{s}$ = 13 TeV and 13.6 TeV with the ATLAS detector Search for Higgs boson pair production in the $\mathrm{b}\overline{\mathrm{b}}$W$^+$W$^-$ decay mode in proton-proton collisions at $\sqrt{s}$ = 13 TeV

Reference 47

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source=pdf_text observed=2026-07-30T18:22:14.597620Z digest=sha256:bb34b35b63f4f1ba7d025959a19a2a14d6a337a1ff5f59a73ebeade7e3485257

Reference 48

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source=pdf_text observed=2026-07-30T18:22:14.672906Z digest=sha256:ea9ae76a5a66185cf3a1f7c1bf8bf2394db3b31fad905a796482ba6990eabbec

Reference 49

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source=pdf_text observed=2026-07-30T18:22:14.749682Z digest=sha256:c9edd4aca9cae7b6855829213cbc81d8ca746007551e51e71c44e71d17e9da24

Reference 50

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source=pdf_text observed=2026-07-30T18:22:14.830549Z digest=sha256:ae5d9044bf98a9462a1b45de2dc426c3d1eabc3b72980e8eb9bf79d9978399a8

Reference 51

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source=pdf_text observed=2026-07-30T18:22:14.916514Z digest=sha256:097556b69dd29acce80900b6fc3ec7869ccab8ea728066fe9be4d2d62e406c6d

Observation 35332f7e-d103-4bd4-9ff4-af5e13745f26 · outbound

This paper cites Study of ZZ and ZH production in the bb$\tau\tau$ final state and search for high-mass spin-0 and spin-1 resonances in proton-proton collisions at $\sqrt{s}$ = 13 TeV.

Improved analysis of non-resonant Higgs boson pair production in the $b\bar{b}\tau^+\tau^-$ final state with $196$ fb$^{-1}$ of data collected at $\sqrt{s}$ = 13 TeV and 13.6 TeV with the ATLAS detector Study of ZZ and ZH production in the bb$\tau\tau$ final state and search for high-mass spin-0 and spin-1 resonances in proton-proton collisions at $\sqrt{s}$ = 13 TeV

Reference 52

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source=pdf_text observed=2026-07-30T18:22:14.999704Z digest=sha256:8287596a5f6497bf03c27dbd0c5ec6d0e5fbcc5dd7edfe85564c4cac2be03e61

Reference 53

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no resolver link, observed 2026-07-30T18:22:15.079213Z

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source=pdf_text observed=2026-07-30T18:22:15.079213Z digest=sha256:3edf4b1812e798737d9c2ecbdd780173a5438d9b6037ca33bc302eb2c087a260

Reference 54

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source=pdf_text observed=2026-07-30T18:22:15.128501Z digest=sha256:171797332d28c0bd91a0425fb00ccd287eb50de4e23a0fbd1a67c52ae1dd1509

Reference 55

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source=pdf_text observed=2026-07-30T18:22:15.204023Z digest=sha256:e9ea07acadc19725f5821e6070236c0df78192039de35dc27467eefe556d1613

Reference 56

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source=pdf_text observed=2026-07-30T18:22:15.283331Z digest=sha256:bec02055e0435d1d562a281fa8abfef2553987d0c2fb43a5a289f45c90d8ec64

Reference 57

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source=pdf_text observed=2026-07-30T18:22:15.367402Z digest=sha256:3522ec3ef5a7e3cfa57a042da52904bbc762d60841feec6b33995febad7f0d9e

Reference 58

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source=pdf_text observed=2026-07-30T18:22:15.445312Z digest=sha256:d8babab68c9008909126e3a9f55e4d80b116e6336d5039ab79ab3d5013a59069

Reference 59

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source=pdf_text observed=2026-07-30T18:22:15.528432Z digest=sha256:bc82af50423d25a581e0aaf2b16cd1227aca33f565a53b25882a2d735866349d

Reference 60

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source=pdf_text observed=2026-07-30T18:22:15.605723Z digest=sha256:b61b1c0ba89d8d3a2175af34f6065266f00a5cc99d4e4683422c5b0e1197495c

Observation eadbd497-e023-4820-82ff-cf784eee4942 · outbound

This paper cites Agostinelli et al.,Geant4– a simulation toolkit, Nucl.

Improved analysis of non-resonant Higgs boson pair production in the $b\bar{b}\tau^+\tau^-$ final state with $196$ fb$^{-1}$ of data collected at $\sqrt{s}$ = 13 TeV and 13.6 TeV with the ATLAS detector Agostinelli et al.,Geant4– a simulation toolkit, Nucl

Reference 61

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source=pdf_text observed=2026-07-30T18:22:15.692921Z digest=sha256:a7e67409bc94063b21c1d1fcf370153dbf6b61a48c88287bb4b9dc9cd6cbc8a6

Reference 62

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source=pdf_text observed=2026-07-30T18:22:15.774243Z digest=sha256:0b0109f1732bfe6d552d18d8023a823e9dd5ee67ff90a5077d0fe85e02985fe2

Reference 63

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source=pdf_text observed=2026-07-30T18:22:15.845943Z digest=sha256:8a2566847477d46a90e3ff5a2263146f4acf5860a96e63d4af429cb1f7e6d341

Reference 64

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source=pdf_text observed=2026-07-30T18:22:15.929918Z digest=sha256:d282949cf0069fa88ac0a6c51c75a301f6adb12604193933baae70715b7638e6

Reference 65

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source=pdf_text observed=2026-07-30T18:22:15.990057Z digest=sha256:17474115e56dcd9e3ceeac43af5990726b68edf4a7ef94df0357ad36852f1f4a

Reference 66

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source=pdf_text observed=2026-07-30T18:22:16.059196Z digest=sha256:c55090555b6b4752c66b378b85f62362ef52b5b013b0c1203a44d9c4f3231d33

Reference 67

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source=pdf_text observed=2026-07-30T18:22:16.152269Z digest=sha256:e93fd1467cb565ea8df180306348705c1580f422d5a0dda67597e272684cbf8b

Reference 68

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source=pdf_text observed=2026-07-30T18:22:16.232584Z digest=sha256:8c704052311a1ef213541f0a7cf2c789232cdfae444ec80252a6d244e984c4ff

Reference 69

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source=pdf_text observed=2026-07-30T18:22:16.323338Z digest=sha256:2145a8cfe75837fbb10ee73a812a86926544c37bc1f1f678a1e2c20020a8bf50

Reference 70

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source=pdf_text observed=2026-07-30T18:22:16.415695Z digest=sha256:854af9c561bbfc9c0363634beeb4bcfe4683e88dd35a2a7f4da36c5bd488f81f

Reference 71

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source=pdf_text observed=2026-07-30T18:22:16.519660Z digest=sha256:dc431a3821756facde38278fced627c1b1ae589e2981c675949e4de3dc8edcda

Reference 72

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source=pdf_text observed=2026-07-30T18:22:16.619244Z digest=sha256:ceaf1a1ed4116a1191466dfaebdd88140ce9ba5533eb9a75785f860249b6401d

Reference 73

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source=pdf_text observed=2026-07-30T18:22:16.675405Z digest=sha256:0ada132098cf3e1b8bccbf885c20c6aebb6a6c6fe7af955cd6f6af7715b8ff4c

Reference 74

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source=pdf_text observed=2026-07-30T18:22:16.770506Z digest=sha256:0daf5d89fa941c5017594b7e473e8822b9f6f05413a5b1b35cc827ab6df7c528

Reference 75

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source=pdf_text observed=2026-07-30T18:22:16.842974Z digest=sha256:f9087c23c81272146b8f07d940a24ed49a382bddb8ac5b64e8a36fafce9f096f

Reference 76

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source=pdf_text observed=2026-07-30T18:22:16.909607Z digest=sha256:0d81f84cd8bb7229fa61480bca97fe560be932d633786dcdbd5956002b9e62c7

Reference 77

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source=pdf_text observed=2026-07-30T18:22:16.999828Z digest=sha256:23d3bd728b1cb71f9f1b425ea5816a1dfa0bafeb2076d0db723c0c82b4c6d4e6

Reference 78

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source=pdf_text observed=2026-07-30T18:22:17.136838Z digest=sha256:29a15576a084ca5dea4b3ff19e1a841bf197c8f1f221f23261ed4c3aeeaaee3b

Reference 79

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source=pdf_text observed=2026-07-30T18:22:17.311460Z digest=sha256:0a2084539b9573587f38a2426afbb74645c09bad629bafc61d0befe9df388b14

Reference 80

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source=pdf_text observed=2026-07-30T18:22:17.418851Z digest=sha256:b1d564ce13785780fbf6583cbaf77e843352298d27d9b25131021ecc15941aaa

Reference 81

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source=pdf_text observed=2026-07-30T18:22:17.546735Z digest=sha256:a81003c511e3e0e8c3cf5729fbacfd97cef6a00cde9aed28c214dfeed374cfda

Reference 82

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source=pdf_text observed=2026-07-30T18:22:17.631954Z digest=sha256:65c2b446170bfb03ed2878ef23d1f95a87da74e646e93065acb23007cf593de8

Reference 83

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source=pdf_text observed=2026-07-30T18:22:17.801432Z digest=sha256:777c21ea464faf73ea872c8173af9a34b4242369f25997f80ad6ea6b856394bf

Reference 84

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no resolver link, observed 2026-07-30T18:22:17.976179Z

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source=pdf_text observed=2026-07-30T18:22:17.976179Z digest=sha256:24aeb4fc6ae4d4deade5264328ebc81896561cb23ffa2172ee09ff1f6e3940e7

Reference 85

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source=pdf_text observed=2026-07-30T18:22:18.083215Z digest=sha256:cd54fcfb98330ede333ebbb6bd149416e97843fdaae2e39f742749e351186602

Reference 86

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source=pdf_text observed=2026-07-30T18:22:18.160278Z digest=sha256:f395656bbca156829911eda0e5745f8750213d5aae54087c1532f69c2453bb1c

Reference 87

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source=pdf_text observed=2026-07-30T18:22:18.338485Z digest=sha256:322c70924d2b76e92bf8cc3e1ce84fee1291833098963c44f8e84a7e80e97c7a

Reference 88

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source=pdf_text observed=2026-07-30T18:22:18.516542Z digest=sha256:40379cba6aad9bf8b1c96ae331511ecac92085700c59bbb4930a50e6bd28f82f

Reference 89

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source=pdf_text observed=2026-07-30T18:22:18.598607Z digest=sha256:803fb784082c152033806d306f68156bf7388ca43c8a9c1bfb4e18b05adbc943

Reference 90

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source=pdf_text observed=2026-07-30T18:22:18.685068Z digest=sha256:ad207803f3704a378e2642456dff0b71be61ddd42761f82b2cf1d07ee1ad4d77

Reference 91

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source=pdf_text observed=2026-07-30T18:22:18.760004Z digest=sha256:0348125c3853515397e87b06b585f65875bb70da1d89b64a1401f9975e147012

Reference 92

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source=pdf_text observed=2026-07-30T18:22:18.847018Z digest=sha256:e21522cc57a0048721f9c19f103cc364a9235510181b13ece3209d2248ddd471

Reference 93

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source=pdf_text observed=2026-07-30T18:22:18.922608Z digest=sha256:77b029bd2877fea3c13ad2fa92cdd8d070e7ee0d00aa1b1434f992a9ce4cb287

Reference 94

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source=pdf_text observed=2026-07-30T18:22:18.946440Z digest=sha256:88854217591941e23eb4ad16e3fa982eae92e4a68bfe4455632e51dd0a09f0c4

Reference 95

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source=pdf_text observed=2026-07-30T18:22:18.977084Z digest=sha256:f5c16fcc185b98ac01709608cee88182f452d22422f60c252db2e257c66a1ed6

Reference 96

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source=pdf_text observed=2026-07-30T18:22:19.116219Z digest=sha256:53a142f0714f5d094a1b50e324cb3326a76da8716eb0245df1737c632536cba1

Reference 97

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source=pdf_text observed=2026-07-30T18:22:19.223827Z digest=sha256:6e05a328f51ba0fe3a47eca549ab25b644cfdaafa9cc03d1e9bea362ed3c9139

Reference 98

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source=pdf_text observed=2026-07-30T18:22:19.346976Z digest=sha256:d72a4c67ffcfd6026a69abe45b3379893adac3689e30c0806df4ff3e661b5b10

Reference 99

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source=pdf_text observed=2026-07-30T18:22:19.454571Z digest=sha256:e09be49d3c4574e478c4970da16d40fbb9a73d4806227672954028e4d1d70131

Reference 100

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source=pdf_text observed=2026-07-30T18:22:19.560516Z digest=sha256:721c139a89bf3fd9ae8194b2163d19dc3121e12722a8aec9895a601e83e07c5a

Pith citing papers

No inbound Pith citation observations are available.