cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.5061/dryad.37mc0
title: Data from: Estimating phenotypic selection in age-structured populations by removing transient fluctuations

description: An extension of the selection differential in the Robertson–Price equation
 for the mean phenotype in an age-structured population is provided.
 Temporal changes in the mean phenotype caused by transient fluctuations in
 the age-distribution and variation in mean phenotype among age classes,
 which can mistakenly be interpreted as selection, will disappear if
 reproductive value weighting is applied. Changes in any weighted mean
 phenotype in an age-structured population may be decomposed into between-
 and within-age class components. Using reproductive value weighting the
 between-age class component becomes pure noise, generated by previous
 genetic drift or fluctuating selection. This component, which we call
 transient quasi-selection, can therefore be omitted when estimating
 age-specific selection on fecundity or viability within age classes. The
 final response can be computed at the time of selection, but can not be
 observed until lifetime reproduction is realized unless the heritability
 is one. The generality of these results is illustrated further by our
 derivation of the selection differential for the continuous time
 age-structured model with general age-dependent weights. A simple
 simulation example as well as estimation of selection components in a
 house sparrow population illustrates the applicability of the theory to
 analyze selection on the mean phenotype in fluctuating age-structured
 populations.
description: House sparrow
 longitudinal dataThe dataset contains
 individual based data on individual survival, reproduction and morphology
 over the years 2002 to 2007 in an island house sparrow
 population.sparrow_aldra_2002-07_2014-05-13.txt
DOI: 10.5061/dryad.ps639
title: Data from: Specificity, rank preference and the colonization of a non-native host plant by the Melissa blue butterfly

description: Animals often express behavioral preferences for different types of food
 or other resources, and these preferences can evolve or shift following
 association with novel food types. Shifts in preference can involve at
 least two phenomena: a change in rank preference or a change in
 specificity. The former corresponds to a change in the order in which
 hosts are preferred, while a shift in specificity can be an increase in
 the tendency to utilize multiple hosts. These possibilities have been
 examined in relatively few systems that include extensive population-level
 replication. The Melissa blue butterfly, Lycaeides melissa, has colonized
 exotic alfalfa, Medicago sativa, throughout western North America. We
 assayed host preferences of 229 females from 10 populations associated
 with novel and native hosts. In four out of five native-associated
 populations, a native host was preferred over the exotic host, while
 preference for a native host characterized only two out of five of the
 alfalfa-associated populations. Across all individuals from
 alfalfa-associated populations, there appears to have been a decrease in
 specificity: females from these populations lay fewer eggs on the native
 host and more eggs on the exotic relative to females from native-host
 populations. However, females from alfalfa-associated populations did not
 lay more eggs on a third plant species, which suggests that preferences
 for specific hosts in this system can potentially be gained and lost
 independently. Geographic variation in oviposition preference in L.
 melissa highlights the value of surveying a large number of populations
 when studying the evolution of a complex behavioral trait.
description: PreferenceDataPreference data across populations and hosts. First column contains population labels as in Fig. 1 of the associated manuscript; the numbers of eggs laid on the three plant types are given in the next columns. Each row corresponds to a single female from a single preference arena.
DOI: 10.17182/hepdata.165445.v1/t1
title: "2.a. Offline Tracking efficiency vs simulated radial position" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: Offline standard tracking efficiency during Run~3 for different tracking iterations, as a function of simulated radial position of the track production vertex. In the figure, $t\bar{t}$ simulation for 2025 conditions and an average PU of 62 is used, and the tracks are required to have $\mathrm{p_T}&gt;0.9$ GeV and $|\eta|&lt;2.5$. The tracking efficiency is defined as the ratio of the simulated tracks (with the aforementioned selection requirements) geometrically matched to a reconstructed track, divided by the total simulated tracks passing the selections.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t2
title: "2.b. HLT Tracking efficiency vs simulated radial position" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: Overall standard tracking efficiency at the HLT during Run~3, as a function of the simulated radial position of the track production vertex. In the figure, $t\bar{t}$ simulation for 2025 conditions and an average PU of 62 is used, and the tracks are required to have $\mathrm{p_T}&gt;0.9$ GeV and $|\eta|&lt;2.5$. The tracking efficiency is defined as the ratio of the simulated tracks (with the aforementioned selection requirements) geometrically matched to a reconstructed track, divided by the total simulated tracks passing the selections.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t3
title: "10.a. MET+IsoTrk efficiency vs Tracker layers with measurement" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: L1T+HLT efficiency of the MET+IsoTrk trigger as a function of the number of tracker layers with valid measurements of the track that pass the offline requirements, in $\tilde{\chi}_{1}^{\pm} \rightarrow \tilde{\chi}_{1}^{0}$+X simulated events for 2022 conditions, where $m_{\tilde{\chi}_{1}^{\pm}}=900$ GeV and $\tilde{\chi}_{1}^{0}$ is nearly mass-degenerate with $\tilde{\chi}_{1}^{\pm}$. The efficiency is shown for LLPs with $c\tau=$ 10, 100, and 1000 cm in black, blue, and red, respectively.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t5
title: "11.a. MET filter efficiency vs PF missing transverse momentum" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: Efficiency of the L1T+HLT $p_{T}^{miss}$ leg as a function of offline reconstructed PF $p_{T}^{miss, \mu \hspace{-0.15cm} /}$ in 2022 data (black), 2023 data (blue), and $W \rightarrow l \nu$ simulation (red).
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t6
title: "11.b. IsoTrk filter efficiency vs PF missing transverse momentum" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: Efficiency of the full HLT path, taking into account only events that already passed through the $p_{T}^{miss}$ leg, as a function of the selected muon $p_{T}$ in 2022 data (black), 2023 data (blue), and $W \rightarrow l \nu$ simulation (red).
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t7
title: "13.a. Disp. tau trigger eff. vs $d_{0}$" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: The L1T+HLT efficiency of the displaced $\tau_\mathrm{h}$ trigger, for simulated $\mathrm{p}\mathrm{p} \to \tilde{\tau}\tilde{\tau},(\tilde{\tau} \to \tau\tilde{\chi}^{0}_{1})$ events, where the $\tilde{\tau}$ has $c\tau = 10$ cm and each $\tau$ decays hadronically. The efficiency is shown for the displaced di-$\tau_\mathrm{h}$ trigger path (blue filled triangles), the previously available $\mathrm{p_{T}^{miss}}$-based paths (orange open circles), the previously available prompt di-$\tau_\mathrm{h}$ paths (purple open squares), the combination of the $\mathrm{p_{T}^{miss}}$-based and prompt di-$\tau_\mathrm{h}$ paths (gray open triangles), and the combination of the $\mathrm{p_{T}^{miss}}$-based, prompt di-$\tau_\mathrm{h}$, and displaced di-$\tau_\mathrm{h}$ paths (red filled circles), using 2022 data-taking conditions. The efficiency is evaluated with respect to generator-level quantities. Efficiency of the highest $\mathrm{p_{T}}$ $\tau$ lepton in the event as a function of the $d_{0}$ (left). Efficiency as a function of $\mathrm{p_{T}^{miss}}$ (right). A selection on the visible component of the generator-level $\tau$ lepton $\mathrm{p_{T}} &gt;$ 30 GeV and its pseudorapidity $|{\eta}| &lt; 2.1$ is applied. The lower panels show the ratio (improvement in \%) of the trigger efficiency given by the combination of the displaced di-$\tau_\mathrm{h}$ trigger path with the $\mathrm{p_{T}^{miss}}$-based and prompt di-$\tau_\mathrm{h}$ paths to that of the combination of the previously available $\mathrm{p_{T}^{miss}}$-based and prompt di-$\tau_\mathrm{h}$ paths.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t8
title: "13.b. Disp. tau trigger eff. vs $\mathrm{p_{T}^{miss}}$" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: The L1T+HLT efficiency of the displaced $\tau_\mathrm{h}$ trigger, for simulated $\mathrm{p}\mathrm{p} \to \tilde{\tau}\tilde{\tau},(\tilde{\tau} \to \tau\tilde{\chi}^{0}_{1})$ events, where the $\tilde{\tau}$ has $c\tau = 10$ cm and each $\tau$ decays hadronically. The efficiency is shown for the displaced di-$\tau_\mathrm{h}$ trigger path (blue filled triangles), the previously available $\mathrm{p_{T}^{miss}}$-based paths (orange open circles), the previously available prompt di-$\tau_\mathrm{h}$ paths (purple open squares), the combination of the $\mathrm{p_{T}^{miss}}$-based and prompt di-$\tau_\mathrm{h}$ paths (gray open triangles), and the combination of the $\mathrm{p_{T}^{miss}}$-based, prompt di-$\tau_\mathrm{h}$, and displaced di-$\tau_\mathrm{h}$ paths (red filled circles), using 2022 data-taking conditions. The efficiency is evaluated with respect to generator-level quantities. Efficiency of the highest $\mathrm{p_{T}}$ $\tau$ lepton in the event as a function of the $d_{0}$ (left). Efficiency as a function of $\mathrm{p_{T}^{miss}}$ (right). A selection on the visible component of the generator-level $\tau$ lepton $\mathrm{p_{T}} &gt;$ 30 GeV and its pseudorapidity $|{\eta}| &lt; 2.1$ is applied. The lower panels show the ratio (improvement in \%) of the trigger efficiency given by the combination of the displaced di-$\tau_\mathrm{h}$ trigger path with the $\mathrm{p_{T}^{miss}}$-based and prompt di-$\tau_\mathrm{h}$ paths to that of the combination of the previously available $\mathrm{p_{T}^{miss}}$-based and prompt di-$\tau_\mathrm{h}$ paths.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t9
title: "14.a. Displaced tau trigger rate vs pileup in 2022" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: Total rate of the displaced $\tau_\mathrm{h}$ trigger for a few representative runs in 2022 data, as a function of PU.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.5281/zenodo.18385493
title: Processed 16S rRNA gene sequencing data of orbital adipose tissue in thyroid-associated ophthalmopathy

description: This dataset contains processed microbiome data derived from 16S rRNA gene sequencing of orbital adipose tissue samples from patients with thyroid-associated ophthalmopathy and non-TAO controls, including decontaminated ASV abundance tables, representative sequences, and sample metadata.
DOI: 10.5281/zenodo.18385494
title: Processed 16S rRNA gene sequencing data of orbital adipose tissue in thyroid-associated ophthalmopathy

description: This dataset contains processed microbiome data derived from 16S rRNA gene sequencing of orbital adipose tissue samples from patients with thyroid-associated ophthalmopathy and non-TAO controls, including decontaminated ASV abundance tables, representative sequences, and sample metadata.
DOI: 10.17182/hepdata.165445.v1/t10
title: "14.b. Displaced tau trigger rate vs pileup in 2023" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: Total rate of the displaced $\tau_\mathrm{h}$ trigger for a few representative runs in 2023 data, as a function of PU.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t11
title: "16.a. Displaced jet HLT $H_{T}$ &gt; 430 GeV efficiency" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: The HLT efficiency for a given event passing the main displaced-jet trigger to satisfy HLT calorimeter $H_{\mathrm{T}}&gt;430~\mathrm{GeV}$ as a function of the offline calorimeter $H_{\mathrm{T}}$. For this trigger, the minimum calorimeter $H_{\mathrm{T}} threshold was 430 GeV in 2022. The measurements are performed in data collected in 2022 (green circles), in 2023 before an update of the HCAL gain values and energy response corrections (black squares), and in 2023 after the update (blue triangles).
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t12
title: "16.b. Displaced jet HLT $H_{T}$ &gt; 390 GeV efficiency" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: The HLT efficiency for a given event passing the main displaced-jet trigger to satisfy HLT calorimeter $H_{\mathrm{T}}&gt;390~\mathrm{GeV}$ as a function of the offline calorimeter $H_{\mathrm{T}}$. For this trigger, the minimum calorimeter $H_{\mathrm{T}} threshold was 390 GeV in 2023 and later. The measurements are performed in data collected in 2022 (green circles), in 2023 before an update of the HCAL gain values and energy response corrections (black squares), and in 2023 after the update (blue triangles).
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t13
title: "17.a. Displaced jet HLT $p_{T}$ &gt; 40 GeV efficiency" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: The HLT efficiency of the main displaced-jet trigger: Efficiency of an offline calorimeter jet to pass the online $\mathrm{p_T}$ requirement in the displaced-jet triggers. In the this plot, the HLT calorimeter jets must have $\mathrm{p_T}&gt;40$ GeV. The efficiency is shown for data collected in 2022 (green squares), in 2023 before an update of the HCAL gains and energy response corrections (black filled circles), and in 2023 after the update (blue open circles). The efficiencies measured with QCD multijet simulations are also shown, for 2022 (red triangles) and 2023 (purple triangles) conditions. These measurements are performed using events collected with a prescaled trigger that requires $\mathrm{H_T} &gt;425$ GeV at the HLT. An offline $\mathrm{H_T} &gt;450$ GeV selection is also applied to ensure the prescaled trigger reaches its plateau. The efficiency is $&gt; 96\%$ when the offline jet has $\mathrm{p_T}&gt;40$ GeV. The efficiency threshold is lower for the later 2023 data following updates to the HCAL energy corrections and readout gains, although the $\mathrm{p_T}$ value at the start of the plateau is unchanged.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.
DOI: 10.17182/hepdata.165445.v1/t15
title: "18. Displaced jet HLT tagging efficiency" of "Strategy and performance of the CMS long-lived particle trigger program in proton-proton collisions at $\sqrt{s}$ = 13.6 TeV"

description: The HLT efficiency of the main displaced-jet trigger for 2022 conditions, for $\mathrm{H} \to \mathrm{S}\mathrm{S}$ signal events where $m_{H}=125$ GeV and $m_{S}=40$ GeV. The per-parton (quark or lepton) HLT displaced-jet tagging efficiency as a function of the generator-level $L_{xy}$ of the parton is shown for displaced b quarks (blue circles), d quarks (purple triangels), and $\tau$ leptons (green squares) with $p_{\mathrm{T}}&gt;40~\mathrm{GeV}$ and $|\eta|&lt;2.0$. Events are required to satisfy the HLT $H_{T} &gt; 430$ GeV requirement.
description: In the physics program of the CMS experiment during the CERN LHC Run 3, which started in 2022, the long-lived particle triggers have been improved and extended to expand the scope of the corresponding searches. These dedicated triggers and their performance are described in this paper, using several theoretical benchmark models that extend the standard model of particle physics. The results are based on proton-proton collision data collected with the CMS detector during 2022--2024 at a center-of-mass energy of 13.6 TeV, corresponding to integrated luminosities of up to 123 ${\mathrm{fb}}^{-1}$.