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        <title>Observation of a New Particle in the Search for the Standard Model Higgs Boson with the ATLAS Detector</title>
        <author>ATLAS Collaboration</author>
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        <p>Tag layer of the DHSS Meta-Tagging Project. The article text is reproduced from the
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        <bibl>
          <title>Observation of a New Particle in the Search for the Standard Model Higgs Boson with the ATLAS Detector</title>
          <date>2012</date>
          <publisher>Physics Letters B / arXiv</publisher>
          
          <idno type="arXiv">1207.7214</idno>
          <idno type="record">atlas2012-higgs</idno>
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          <note type="rights">arxiv-open</note>
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        <label>existence</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t1" type="phenomenon" ana="#phenomenon" resp="#paper">
        <label>Standard Model Higgs boson search</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t2" type="method" ana="#method" resp="#paper">
        <label>experiment</label>
        <term>experiment</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t3" type="mechanisms" ana="#mechanisms[0]" resp="#tagger" cert="0.85">
        <label>mechanisms</label>
        <term>the whole search is reduced to ONE parameter of interest - a signal strength that scales the predicted signal - and it is defined so that zero is the background-only hypothesis and one is the Standard Model Higgs signal, so the hypothesis under test is a value of that one factor</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t4" type="mechanisms" ana="#mechanisms[1]" resp="#tagger" cert="0.85">
        <label>mechanisms</label>
        <term>hypothesised values of that strength are tested with a profile likelihood ratio, which extracts the signal strength from a full likelihood fit whose function INCLUDES all the parameters describing the systematic uncertainties and their correlations</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t5" type="mechanisms" ana="#mechanisms[2]" resp="#tagger" cert="0.85">
        <label>mechanisms</label>
        <term>exclusion is decided by a stated numerical rule rather than by judgement: a signal strength is excluded at 95% confidence when its CLs value falls below 5%, and a Standard Model Higgs of a given mass counts as excluded when the value one is excluded at that mass</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t6" type="mechanisms" ana="#mechanisms[3]" resp="#tagger" cert="0.95">
        <label>mechanisms</label>
        <term>the size of an excess is first expressed as the probability that background alone could produce a fluctuation at least that large, and only then converted into the equivalent number of standard deviations - the local significance</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t7" type="mechanisms" ana="#mechanisms[4]" resp="#tagger" cert="0.95">
        <label>mechanisms</label>
        <term>that local number is then corrected for having searched a whole mass range rather than one point: the ratio of global to local probability is the trials factor, and the paper states what it depends on - the range of hypotheses considered, the mass resolutions of the channels combined, and the size of the excess itself</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t8" type="mechanisms" ana="#mechanisms[5]" resp="#tagger" cert="0.85">
        <label>mechanisms</label>
        <term>the tests are run in steps across the hypothesised mass rather than at one chosen point, and the asymptotic approximation the results rest on is not assumed to hold - it is validated by a separately described method</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t9" type="mechanisms" ana="#mechanisms[6]" resp="#tagger" cert="0.85">
        <label>mechanisms</label>
        <term>the combination across channels is built on the same single signal strength together with an explicit identification of which nuisance parameters correspond to the CORRELATED sources of systematic uncertainty</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>mechanisms</label>
        <term>the jet energy scale and resolution are handled by a deliberately simplified scheme - independent nuisance parameters attached to final states with materially different selections and process sensitivity - and the simplification is defended by measurement: the results were found insensitive to the assumptions made about how those sources correlate</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t11" type="limitations" ana="#limitations[0]" resp="#tagger">
        <label>The data establish a new neutral boson but are insufficient to determine whether it is in fact the Standard Model Higgs boson.</label>
        <note>what this limits: the identification of the particle, as distinct from its discovery: THESE RESULTS ARE COMPATIBLE WITH THE HYPOTHESIS THAT THE NEW PARTICLE IS THE STANDARD MODEL HIGGS BOSON, [but] MORE DATA ARE NEEDED TO ASSESS ITS NATURE IN DETAIL</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>Increased pile-up degraded missing-transverse-momentum resolution so badly that the same-flavour WW final states had to be dropped from the 8 TeV analysis.</label>
        <note>what this limits: the 8 TeV WW analysis specifically: SINCE THE e-mu CHANNEL PROVIDES MOST OF THE SENSITIVITY OF THE SEARCH, ONLY THIS FINAL STATE IS USED - pile-up degraded the resolution the same-flavour states needed</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t13" type="limitations" ana="#limitations[2]" resp="#tagger" cert="1.0">
        <label>The same excess carries three significances: 5.9 sigma locally, about 5.1 sigma globally over 110-600 GeV, and 5.3 sigma over a narrower range whose bounds are lost to figure text in this staged copy.</label>
        <note>what this limits: the 5.9 sigma figure as the discovery significance: the paper gives about 5.1 sigma globally over 110-600 GeV, and a different value again over a narrower range</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>The correction from local to global significance is stated to depend on the mass range searched, the channels&#x27; mass resolutions, and the size of the excess.</label>
        <note>what this limits: comparing significances across searches: the trials factor depends on the range of hypotheses considered, so the same excess yields different global significances</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t15" type="limitations" ana="#limitations[4]" resp="#tagger" cert="1.0">
        <label>Compatibility with the Standard Model expectation is quantified at the 1.5 sigma level rather than asserted.</label>
        <note>what this limits: the result as agreement with the Standard Model: the paper quantifies the compatibility at 1.5 sigma</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t16" type="limitations" ana="#limitations[5]" resp="#tagger" cert="1.0">
        <label>Only the spin-1 hypothesis is addressed, and only by the diphoton observation.</label>
        <note>what this limits: the new particle&#x27;s spin: only spin-1 is disfavoured here, by the diphoton observation alone</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>statistical significance testing (p-values, sigma levels) used to establish the discovery of a new particle against background fluctuations</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t18" type="controls" ana="#controls[0]" resp="#tagger" cert="0.9">
        <label>control and validation regions built with the signal-region selections but with criteria reversed or modified, so the samples are depleted of signal</label>
        <note>eliminates: a background estimate taken from the same events as the signal - the reversed criteria give regions where the signal cannot be, and the background can therefore be measured rather than assumed · outcome (stated by the tagger, no quotation): held</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>validation regions kept separate from the control regions used to normalise the backgrounds, with the paper stating which does which</label>
        <note>eliminates: checking the background model on the very regions that were used to fit it - the distinction is what keeps the check independent of the fit · outcome (stated by the tagger, no quotation): held</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t20" type="controls" ana="#controls[2]" resp="#tagger" cert="0.9">
        <label>data-driven estimation of the numbers of two-photon, photon-jet and jet-jet events in the selected sample</label>
        <note>eliminates: reliance on simulation for the backgrounds hardest to simulate - jets faking photons is precisely where Monte Carlo is least trusted, so that component is measured from data · outcome (stated by the tagger, no quotation): held</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t21" type="controls" ana="#controls[3]" resp="#tagger" cert="0.9">
        <label>a trials factor applied to convert the local probability to a global one, correcting for the range of Higgs mass hypotheses searched</label>
        <note>eliminates: having looked in many places and reported the luckiest - the look-elsewhere correction is what makes the quoted significance a statement about the search rather than about one bin · outcome (stated by the tagger, no quotation): held</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>local significance</label>
        <term>local significance</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t23" type="concepts" ana="#concepts[5]" resp="#paper">
        <label>global significance</label>
        <term>global significance</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>trials factor</label>
        <term>trials factor</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t25" type="concepts" ana="#concepts[7]" resp="#paper">
        <label>Standard Model Higgs boson</label>
        <term>Standard Model Higgs boson</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t26" type="senses" ana="#senses[0]" resp="#tagger" cert="1.0">
        <label>local significance - the number of standard deviations corresponding to the background producing a fluctuation at least as large as the excess observed, at one mass</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t27" type="senses" ana="#senses[1]" resp="#tagger" cert="1.0">
        <label>global significance - the same excess corrected for having searched a whole mass range, which lowers 5.9 sigma to approximately 5.1 sigma over 110-600 GeV</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t28" type="senses" ana="#senses[2]" resp="#tagger" cert="1.0">
        <label>trials factor - the ratio of global to local probability, larger the wider the range of hypotheses searched</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t29" type="claim_relations" ana="#claim_relations[0]" resp="#tagger">
        <label>builds-on → the Standard Model Higgs prediction</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t30" type="claim_relations" ana="#claim_relations[1]" resp="#tagger">
        <label>extends → the previous ATLAS H-&gt;ZZ(*)-&gt;4l analysis, Ref. [83]</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
      </span>
      <span xml:id="t31" type="concept_edges" ana="#concept_edges[0]" resp="#tagger">
        <label>global significance —distinct-from→ local significance</label>
        <term>global significance</term>
        <term>local significance</term>
        <note>strength of the relation: 1
Audit 2026-09-28: DOUBTFUL - read against its full span and kept, but the span reports the global significance of a local excess; distinct-from is loose.</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t32" type="concept_edges" ana="#concept_edges[1]" resp="#tagger">
        <label>trials factor —part-of→ global significance</label>
        <term>trials factor</term>
        <term>global significance</term>
        <note>strength of the relation: 1
Audit 2026-09-28: DOUBTFUL - read against its full span and kept, but the trials factor is the RATIO of global to local probabilities, used to correct; part-of is loose.</note>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t33" type="content_tags" ana="#content_tags.quantities[0]" resp="#tagger">
        <label>5.9 — discovery significance of the new boson</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t34" type="content_tags" ana="#content_tags.quantities[1]" resp="#tagger">
        <label>126.0 — measured mass of the new neutral boson</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t35" type="content_tags" ana="#content_tags.quantities[2]" resp="#tagger">
        <label>7 — 2011 collision centre-of-mass energy</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t36" type="content_tags" ana="#content_tags.quantities[3]" resp="#tagger">
        <label>124-126 — mass region of the 2011 excess</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t37" type="content_tags" ana="#content_tags.quantities[4]" resp="#tagger">
        <label>2.9 and 3.1 — ATLAS/CMS 2011 excess significances</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t38" type="content_tags" ana="#content_tags.quantities[5]" resp="#tagger">
        <label>~10 to ~20 — pile-up in 7 TeV vs 8 TeV data</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t39" type="content_tags" ana="#content_tags.findings[1]" resp="#tagger">
        <label>the observation reaches 5.9 sigma significance</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t40" type="content_tags" ana="#content_tags.findings[3]" resp="#tagger">
        <label>the Higgs was the only SM particle not yet observed</label>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t41" type="content_tags" ana="#content_tags.variables[0]" resp="#tagger">
        <label>Higgs boson mass mH</label>
        <term>Higgs boson mass mH</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t42" type="content_tags" ana="#content_tags.variables[1]" resp="#tagger">
        <label>centre-of-mass energy √s</label>
        <term>centre-of-mass energy √s</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <span xml:id="t43" type="content_tags" ana="#content_tags.variables[2]" resp="#tagger">
        <label>integrated luminosity</label>
        <term>integrated luminosity</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>pile-up</label>
        <term>pile-up</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>SM Higgs boson</label>
        <term>SM Higgs boson</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>Standard Model</label>
        <term>Standard Model</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>pile-up</label>
        <term>pile-up</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <label>p-value</label>
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        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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        <term>statistical-power</term>
        <note type="quotation-withheld">Quotation withheld because this record is not cleared for redistribution.</note>
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      <p><note type="rights">The full text of this article is not redistributable, so it is
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      grounding status remain. The article itself is at https://arxiv.org/abs/1207.7214.</note></p>
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