#higgs — Public Fediverse posts
Live and recent posts from across the Fediverse tagged #higgs, aggregated by home.social.
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🙈 New preprint, Part V: *What the Higgs Potential Cannot See*.
If you build gauge–Higgs unification models: there is a discrete choice you may be scanning over for nothing. On \(T^2/\mathbb{Z}_2\) each bulk multiplet carries boundary signs \(\eta_0,\eta_1\). For a whole class of bulk matter, the product \(\eta=\eta_0\eta_1\) has no observable consequence in the Higgs sector at one loop. Not suppressed. Identically zero.
Why. The one-loop Wilson-line potential is one operator traced twice. Even windings give a graded dimension, odd windings an index:
\[\Sigma_\lambda=s_\lambda(1,1,t,t^{-1}),\qquad D_\lambda=s_\lambda(1,-1,t,t^{-1}),\]
and AHMN's \(\{A+B(-1)^{k_2}\}\) is exactly \((\Sigma\pm D)/2\). \(\Sigma\) has non-negative coefficients and can never cancel; \(D\) can. η multiplies \(D\) and nothing else — so η is invisible exactly where \(D_\lambda\equiv 0\).Which matter is blind is a parity condition you read off the Young diagram: \(\lambda_1\not\equiv\lambda_2\not\equiv\lambda_3\not\equiv\lambda_4\), or \(\lambda_i+\lambda_{5-i}=c\) odd. Counted in closed form — \(\lceil (k+1)^2/2\rceil\) at \(\lambda_1=2k+1\), none for \(\lambda_1\) even — and machine-checked in Lean 4, sorry-free. A second, disjoint cause: only \(\lfloor (N+1)^2/2\rfloor\) of the \((N+1)^2\) boundary-condition classes of \(SU(N)\) have a coset sector at all, for every \(N\).
Anchored, not fitted: twelve printed coefficients of arXiv:2312.08608 come out exactly, and two further published potentials follow from the same mode counts.
📄 https://doi.org/10.5281/zenodo.21727094
💻 https://github.com/karlesmarin/higgs-blind-class#Physics #ParticlePhysics #HEP #BSM #Higgs #ExtraDimensions #Lean4
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🙈 New preprint, Part V: *What the Higgs Potential Cannot See*.
If you build gauge–Higgs unification models: there is a discrete choice you may be scanning over for nothing. On \(T^2/\mathbb{Z}_2\) each bulk multiplet carries boundary signs \(\eta_0,\eta_1\). For a whole class of bulk matter, the product \(\eta=\eta_0\eta_1\) has no observable consequence in the Higgs sector at one loop. Not suppressed. Identically zero.
Why. The one-loop Wilson-line potential is one operator traced twice. Even windings give a graded dimension, odd windings an index:
\[\Sigma_\lambda=s_\lambda(1,1,t,t^{-1}),\qquad D_\lambda=s_\lambda(1,-1,t,t^{-1}),\]
and AHMN's \(\{A+B(-1)^{k_2}\}\) is exactly \((\Sigma\pm D)/2\). \(\Sigma\) has non-negative coefficients and can never cancel; \(D\) can. η multiplies \(D\) and nothing else — so η is invisible exactly where \(D_\lambda\equiv 0\).Which matter is blind is a parity condition you read off the Young diagram: \(\lambda_1\not\equiv\lambda_2\not\equiv\lambda_3\not\equiv\lambda_4\), or \(\lambda_i+\lambda_{5-i}=c\) odd. Counted in closed form — \(\lceil (k+1)^2/2\rceil\) at \(\lambda_1=2k+1\), none for \(\lambda_1\) even — and machine-checked in Lean 4, sorry-free. A second, disjoint cause: only \(\lfloor (N+1)^2/2\rfloor\) of the \((N+1)^2\) boundary-condition classes of \(SU(N)\) have a coset sector at all, for every \(N\).
Anchored, not fitted: twelve printed coefficients of arXiv:2312.08608 come out exactly, and two further published potentials follow from the same mode counts.
📄 https://doi.org/10.5281/zenodo.21727094
💻 https://github.com/karlesmarin/higgs-blind-class#Physics #ParticlePhysics #HEP #BSM #Higgs #ExtraDimensions #Lean4
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🙈 New preprint, Part V: *What the Higgs Potential Cannot See*.
If you build gauge–Higgs unification models: there is a discrete choice you may be scanning over for nothing. On \(T^2/\mathbb{Z}_2\) each bulk multiplet carries boundary signs \(\eta_0,\eta_1\). For a whole class of bulk matter, the product \(\eta=\eta_0\eta_1\) has no observable consequence in the Higgs sector at one loop. Not suppressed. Identically zero.
Why. The one-loop Wilson-line potential is one operator traced twice. Even windings give a graded dimension, odd windings an index:
\[\Sigma_\lambda=s_\lambda(1,1,t,t^{-1}),\qquad D_\lambda=s_\lambda(1,-1,t,t^{-1}),\]
and AHMN's \(\{A+B(-1)^{k_2}\}\) is exactly \((\Sigma\pm D)/2\). \(\Sigma\) has non-negative coefficients and can never cancel; \(D\) can. η multiplies \(D\) and nothing else — so η is invisible exactly where \(D_\lambda\equiv 0\).Which matter is blind is a parity condition you read off the Young diagram: \(\lambda_1\not\equiv\lambda_2\not\equiv\lambda_3\not\equiv\lambda_4\), or \(\lambda_i+\lambda_{5-i}=c\) odd. Counted in closed form — \(\lceil (k+1)^2/2\rceil\) at \(\lambda_1=2k+1\), none for \(\lambda_1\) even — and machine-checked in Lean 4, sorry-free. A second, disjoint cause: only \(\lfloor (N+1)^2/2\rfloor\) of the \((N+1)^2\) boundary-condition classes of \(SU(N)\) have a coset sector at all, for every \(N\).
Anchored, not fitted: twelve printed coefficients of arXiv:2312.08608 come out exactly, and two further published potentials follow from the same mode counts.
📄 https://doi.org/10.5281/zenodo.21727094
💻 https://github.com/karlesmarin/higgs-blind-class#Physics #ParticlePhysics #HEP #BSM #Higgs #ExtraDimensions #Lean4
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🙈 New preprint, Part V: *What the Higgs Potential Cannot See*.
If you build gauge–Higgs unification models: there is a discrete choice you may be scanning over for nothing. On \(T^2/\mathbb{Z}_2\) each bulk multiplet carries boundary signs \(\eta_0,\eta_1\). For a whole class of bulk matter, the product \(\eta=\eta_0\eta_1\) has no observable consequence in the Higgs sector at one loop. Not suppressed. Identically zero.
Why. The one-loop Wilson-line potential is one operator traced twice. Even windings give a graded dimension, odd windings an index:
\[\Sigma_\lambda=s_\lambda(1,1,t,t^{-1}),\qquad D_\lambda=s_\lambda(1,-1,t,t^{-1}),\]
and AHMN's \(\{A+B(-1)^{k_2}\}\) is exactly \((\Sigma\pm D)/2\). \(\Sigma\) has non-negative coefficients and can never cancel; \(D\) can. η multiplies \(D\) and nothing else — so η is invisible exactly where \(D_\lambda\equiv 0\).Which matter is blind is a parity condition you read off the Young diagram: \(\lambda_1\not\equiv\lambda_2\not\equiv\lambda_3\not\equiv\lambda_4\), or \(\lambda_i+\lambda_{5-i}=c\) odd. Counted in closed form — \(\lceil (k+1)^2/2\rceil\) at \(\lambda_1=2k+1\), none for \(\lambda_1\) even — and machine-checked in Lean 4, sorry-free. A second, disjoint cause: only \(\lfloor (N+1)^2/2\rfloor\) of the \((N+1)^2\) boundary-condition classes of \(SU(N)\) have a coset sector at all, for every \(N\).
Anchored, not fitted: twelve printed coefficients of arXiv:2312.08608 come out exactly, and two further published potentials follow from the same mode counts.
📄 https://doi.org/10.5281/zenodo.21727094
💻 https://github.com/karlesmarin/higgs-blind-class#Physics #ParticlePhysics #HEP #BSM #Higgs #ExtraDimensions #Lean4
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🙈 New preprint, Part V: *What the Higgs Potential Cannot See*.
If you build gauge–Higgs unification models: there is a discrete choice you may be scanning over for nothing. On \(T^2/\mathbb{Z}_2\) each bulk multiplet carries boundary signs \(\eta_0,\eta_1\). For a whole class of bulk matter, the product \(\eta=\eta_0\eta_1\) has no observable consequence in the Higgs sector at one loop. Not suppressed. Identically zero.
Why. The one-loop Wilson-line potential is one operator traced twice. Even windings give a graded dimension, odd windings an index:
\[\Sigma_\lambda=s_\lambda(1,1,t,t^{-1}),\qquad D_\lambda=s_\lambda(1,-1,t,t^{-1}),\]
and AHMN's \(\{A+B(-1)^{k_2}\}\) is exactly \((\Sigma\pm D)/2\). \(\Sigma\) has non-negative coefficients and can never cancel; \(D\) can. η multiplies \(D\) and nothing else — so η is invisible exactly where \(D_\lambda\equiv 0\).Which matter is blind is a parity condition you read off the Young diagram: \(\lambda_1\not\equiv\lambda_2\not\equiv\lambda_3\not\equiv\lambda_4\), or \(\lambda_i+\lambda_{5-i}=c\) odd. Counted in closed form — \(\lceil (k+1)^2/2\rceil\) at \(\lambda_1=2k+1\), none for \(\lambda_1\) even — and machine-checked in Lean 4, sorry-free. A second, disjoint cause: only \(\lfloor (N+1)^2/2\rfloor\) of the \((N+1)^2\) boundary-condition classes of \(SU(N)\) have a coset sector at all, for every \(N\).
Anchored, not fitted: twelve printed coefficients of arXiv:2312.08608 come out exactly, and two further published potentials follow from the same mode counts.
📄 https://doi.org/10.5281/zenodo.21727094
💻 https://github.com/karlesmarin/higgs-blind-class#Physics #ParticlePhysics #HEP #BSM #Higgs #ExtraDimensions #Lean4
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I have just received a spam e-mail from a purported journal editor, addressed to “Dear Dr. Higgs”.
That’s a new one!
#spam #Higgs #HiggsBoson #Physics #journal #AcademicChatter #Research
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I have just received a spam e-mail from a purported journal editor, addressed to “Dear Dr. Higgs”.
That’s a new one!
#spam #Higgs #HiggsBoson #Physics #journal #AcademicChatter #Research
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I have just received a spam e-mail from a purported journal editor, addressed to “Dear Dr. Higgs”.
That’s a new one!
#spam #Higgs #HiggsBoson #Physics #journal #AcademicChatter #Research
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I have just received a spam e-mail from a purported journal editor, addressed to “Dear Dr. Higgs”.
That’s a new one!
#spam #Higgs #HiggsBoson #Physics #journal #AcademicChatter #Research
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#physics 14 years ago, #CERN announced evidence for the existence of the #Higgs #boson https://english.netmassimo.com/2012/07/04/cern-announced-evidence-for-the-existance-of-the-higgs-boson/
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#physics 14 years ago, #CERN announced evidence for the existence of the #Higgs #boson https://english.netmassimo.com/2012/07/04/cern-announced-evidence-for-the-existance-of-the-higgs-boson/
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#physics 14 years ago, #CERN announced evidence for the existence of the #Higgs #boson https://english.netmassimo.com/2012/07/04/cern-announced-evidence-for-the-existance-of-the-higgs-boson/
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#physics 14 years ago, #CERN announced evidence for the existence of the #Higgs #boson https://english.netmassimo.com/2012/07/04/cern-announced-evidence-for-the-existance-of-the-higgs-boson/
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#physics 14 years ago, #CERN announced evidence for the existence of the #Higgs #boson https://english.netmassimo.com/2012/07/04/cern-announced-evidence-for-the-existance-of-the-higgs-boson/
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Le CERN lance le projet HiLumi LHC pour augmenter fortement les collisions et mieux étudier la matière noire et le boson de Higgs.
www.france24.com/fr/info-en-c...
#CERN #HiLumiLHC #Physique #Science #Higgs #MatièreNoire
Le plus grand accélérateur de ... -
Le CERN lance le projet HiLumi LHC pour augmenter fortement les collisions et mieux étudier la matière noire et le boson de Higgs.
www.france24.com/fr/info-en-c...
#CERN #HiLumiLHC #Physique #Science #Higgs #MatièreNoire
Le plus grand accélérateur de ... -
Le CERN lance le projet HiLumi LHC pour augmenter fortement les collisions et mieux étudier la matière noire et le boson de Higgs.
www.france24.com/fr/info-en-c...
#CERN #HiLumiLHC #Physique #Science #Higgs #MatièreNoire
Le plus grand accélérateur de ... -
Le CERN lance le projet HiLumi LHC pour augmenter fortement les collisions et mieux étudier la matière noire et le boson de Higgs.
www.france24.com/fr/info-en-c...
#CERN #HiLumiLHC #Physique #Science #Higgs #MatièreNoire
Le plus grand accélérateur de ... -
Le CERN lance le projet HiLumi LHC pour augmenter fortement les collisions et mieux étudier la matière noire et le boson de Higgs.
www.france24.com/fr/info-en-c...
#CERN #HiLumiLHC #Physique #Science #Higgs #MatièreNoire
Le plus grand accélérateur de ... -
https://www.europesays.com/uk/1046458/ François Englert, Nobelist Who Helped Predict the ‘God Particle,’ Dies at 93 #Brout #Deaths(Obituaries) #Englert #Francois #Higgs #HiggsBoson #NobelPrizes #PeterWare #Physics #Research #Robert(19282011) #Science #UK #UnitedKingdom
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François Englert, Nobelist Who Helped Predict the ‘God Particle,’ Dies at 93
On July 4, 2012, scientists packed a large hall at the European Organization for Nuclear Research, also known…
#NewsBeep #News #Physics #Brout #Deaths(Obituaries) #Englert #Francois #Higgs #HiggsBoson #NobelPrizes #PeterWare #research #Robert(1928-2011) #Science #UK #UnitedKingdom
https://www.newsbeep.com/uk/651325/ -
https://www.europesays.com/ie/546377/ François Englert, Nobelist Who Helped Predict the ‘God Particle,’ Dies at 93 #Brout #Deaths(Obituaries) #Éire #FrancoisEnglert #Higgs #HiggsBoson #IE #Ireland #PeterWare #Physics #Research #Robert(19282011) #Science
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#UnDiaComoHoy 29 de mayo de 1929 nace Peter #Higgs, #físico británico, premio #Nobel de #física en 2013
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#UnDiaComoHoy 29 de mayo de 1929 nace Peter #Higgs, #físico británico, premio #Nobel de #física en 2013
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#UnDiaComoHoy 29 de mayo de 1929 nace Peter #Higgs, #físico británico, premio #Nobel de #física en 2013
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Une #anomalie au #LHC pourrait annoncer une percée majeure après le #boson de #Higgs www.futura-sciences.com/sciences/act...
Une anomalie au LHC pourrait a... -
Une #anomalie au #LHC pourrait annoncer une percée majeure après le #boson de #Higgs
Un des détecteurs géants du #LHC, le grand collisionneur de #proton du #Cern reproduisant certaines des conditions du #BigBang, continue à livrer d'intrigantes indications en faveur d'une #nouvelle #physique encore inconnue
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Une #anomalie au #LHC pourrait annoncer une percée majeure après le #boson de #Higgs
Un des détecteurs géants du #LHC, le grand collisionneur de #proton du #Cern reproduisant certaines des conditions du #BigBang, continue à livrer d'intrigantes indications en faveur d'une #nouvelle #physique encore inconnue
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Une #anomalie au #LHC pourrait annoncer une percée majeure après le #boson de #Higgs
Un des détecteurs géants du #LHC, le grand collisionneur de #proton du #Cern reproduisant certaines des conditions du #BigBang, continue à livrer d'intrigantes indications en faveur d'une #nouvelle #physique encore inconnue
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Une #anomalie au #LHC pourrait annoncer une percée majeure après le #boson de #Higgs
Un des détecteurs géants du #LHC, le grand collisionneur de #proton du #Cern reproduisant certaines des conditions du #BigBang, continue à livrer d'intrigantes indications en faveur d'une #nouvelle #physique encore inconnue
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Une #anomalie au #LHC pourrait annoncer une percée majeure après le #boson de #Higgs
Un des détecteurs géants du #LHC, le grand collisionneur de #proton du #Cern reproduisant certaines des conditions du #BigBang, continue à livrer d'intrigantes indications en faveur d'une #nouvelle #physique encore inconnue
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https://www.europesays.com/be-nl/?p=32658 Voorzichtige aanwijzingen voor bestaan van dubbel-higgs gebeurtenissen #Atlas #BE #België #Belgium #CERN #deeltje #experiment #higgs #Science #ScienceAndTechnology #ScienceAndTechnology #Technologie #Technology #Wetenschap #WetenschapEnTechnologie #WetenschapTechnologie
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Just completed my by far most difficult lecture ever with astronomers - get them a sense of the #Higgs mechanism, of the Higgs boson and of the Higgs field in one hour, after a couple of weeks of shallow overview of the Standard Model.
Not sure how it went, but I prepared for a couple of weeks like for a job interview, and my mind exploded 🤯
It won't even be in the final exam, but I tried it first time this year.
Done, exhausting, also because I am not qualified for this.
#physics #science -
Just completed my by far most difficult lecture ever with astronomers - get them a sense of the #Higgs mechanism, of the Higgs boson and of the Higgs field in one hour, after a couple of weeks of shallow overview of the Standard Model.
Not sure how it went, but I prepared for a couple of weeks like for a job interview, and my mind exploded 🤯
It won't even be in the final exam, but I tried it first time this year.
Done, exhausting, also because I am not qualified for this.
#physics #science -
Just completed my by far most difficult lecture ever with astronomers - get them a sense of the #Higgs mechanism, of the Higgs boson and of the Higgs field in one hour, after a couple of weeks of shallow overview of the Standard Model.
Not sure how it went, but I prepared for a couple of weeks like for a job interview, and my mind exploded 🤯
It won't even be in the final exam, but I tried it first time this year.
Done, exhausting, also because I am not qualified for this.
#physics #science -
Just completed my by far most difficult lecture ever with astronomers - get them a sense of the #Higgs mechanism, of the Higgs boson and of the Higgs field in one hour, after a couple of weeks of shallow overview of the Standard Model.
Not sure how it went, but I prepared for a couple of weeks like for a job interview, and my mind exploded 🤯
It won't even be in the final exam, but I tried it first time this year.
Done, exhausting, also because I am not qualified for this.
#physics #science -
Just completed my by far most difficult lecture ever with astronomers - get them a sense of the #Higgs mechanism, of the Higgs boson and of the Higgs field in one hour, after a couple of weeks of shallow overview of the Standard Model.
Not sure how it went, but I prepared for a couple of weeks like for a job interview, and my mind exploded 🤯
It won't even be in the final exam, but I tried it first time this year.
Done, exhausting, also because I am not qualified for this.
#physics #science -
Physicist @[email protected] of @[email protected], who aided in the #Higgs discovery, cautions that not every anomaly matters. “There’s an infinite number of ways the data can look different,” he says. The challenge is finding a “Goldilocks” balance between noise and real physics. (4/8)
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#merrychristmas from earth in this Quantum Foam location from my #physics Christmas tree working on Higgs Field #E8xE8 and Why things weigh what they do and atomic shells fill the way they do from first principle. #stringtheory #quantumphysics #Higgs #fundamentalparticles
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#merrychristmas from earth in this Quantum Foam location from my #physics Christmas tree working on Higgs Field #E8xE8 and Why things weigh what they do and atomic shells fill the way they do from first principle. #stringtheory #quantumphysics #Higgs #fundamentalparticles
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#merrychristmas from earth in this Quantum Foam location from my #physics Christmas tree working on Higgs Field #E8xE8 and Why things weigh what they do and atomic shells fill the way they do from first principle. #stringtheory #quantumphysics #Higgs #fundamentalparticles
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#merrychristmas from earth in this Quantum Foam location from my #physics Christmas tree working on Higgs Field #E8xE8 and Why things weigh what they do and atomic shells fill the way they do from first principle. #stringtheory #quantumphysics #Higgs #fundamentalparticles
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#merrychristmas from earth in this Quantum Foam location from my #physics Christmas tree working on Higgs Field #E8xE8 and Why things weigh what they do and atomic shells fill the way they do from first principle. #stringtheory #quantumphysics #Higgs #fundamentalparticles
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Mithilfe von innovativen Großsimulationen auf verschiedenen Supercomputern ist es Forschern der #UniMainz gelungen, neue Erkenntnisse im Bereich der #Physik der starken Wechselwirkung zu gewinnen. Wissenschaftler vom #ExzellenzclusterPRISMA+ haben auf Grundlage der #Quantenchromodynamik mit bisher unerreichter Präzision die Wechselwirkung des Pions mit dem #Higgs-Feld berechnet 👉 https://presse.uni-mainz.de/computersimulationen-beschreiben-teilcheneigenschaften-mit-beispielloser-praezision/
#Physik #Teilchenphysik #Supercomputer #Hochleistungsrechner #StarkeWechselwirkung #Quarks
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Mithilfe von innovativen Großsimulationen auf verschiedenen Supercomputern ist es Forschern der #UniMainz gelungen, neue Erkenntnisse im Bereich der #Physik der starken Wechselwirkung zu gewinnen. Wissenschaftler vom #ExzellenzclusterPRISMA+ haben auf Grundlage der #Quantenchromodynamik mit bisher unerreichter Präzision die Wechselwirkung des Pions mit dem #Higgs-Feld berechnet 👉 https://presse.uni-mainz.de/computersimulationen-beschreiben-teilcheneigenschaften-mit-beispielloser-praezision/
#Physik #Teilchenphysik #Supercomputer #Hochleistungsrechner #StarkeWechselwirkung #Quarks
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Mithilfe von innovativen Großsimulationen auf verschiedenen Supercomputern ist es Forschern der #UniMainz gelungen, neue Erkenntnisse im Bereich der #Physik der starken Wechselwirkung zu gewinnen. Wissenschaftler vom #ExzellenzclusterPRISMA+ haben auf Grundlage der #Quantenchromodynamik mit bisher unerreichter Präzision die Wechselwirkung des Pions mit dem #Higgs-Feld berechnet 👉 https://presse.uni-mainz.de/computersimulationen-beschreiben-teilcheneigenschaften-mit-beispielloser-praezision/
#Physik #Teilchenphysik #Supercomputer #Hochleistungsrechner #StarkeWechselwirkung #Quarks
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Mithilfe von innovativen Großsimulationen auf verschiedenen Supercomputern ist es Forschern der #UniMainz gelungen, neue Erkenntnisse im Bereich der #Physik der starken Wechselwirkung zu gewinnen. Wissenschaftler vom #ExzellenzclusterPRISMA+ haben auf Grundlage der #Quantenchromodynamik mit bisher unerreichter Präzision die Wechselwirkung des Pions mit dem #Higgs-Feld berechnet 👉 https://presse.uni-mainz.de/computersimulationen-beschreiben-teilcheneigenschaften-mit-beispielloser-praezision/
#Physik #Teilchenphysik #Supercomputer #Hochleistungsrechner #StarkeWechselwirkung #Quarks
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Mithilfe von innovativen Großsimulationen auf verschiedenen Supercomputern ist es Forschern der #UniMainz gelungen, neue Erkenntnisse im Bereich der #Physik der starken Wechselwirkung zu gewinnen. Wissenschaftler vom #ExzellenzclusterPRISMA+ haben auf Grundlage der #Quantenchromodynamik mit bisher unerreichter Präzision die Wechselwirkung des Pions mit dem #Higgs-Feld berechnet 👉 https://presse.uni-mainz.de/computersimulationen-beschreiben-teilcheneigenschaften-mit-beispielloser-praezision/
#Physik #Teilchenphysik #Supercomputer #Hochleistungsrechner #StarkeWechselwirkung #Quarks
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One of my favourite things was the specially labelled bottle of champagne my colleague, Aidan, put together in anticipation of this day. It was drunk with great delight, I am told.
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One of my favourite things was the specially labelled bottle of champagne my colleague, Aidan, put together in anticipation of this day. It was drunk with great delight, I am told.
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One of my favourite things was the specially labelled bottle of champagne my colleague, Aidan, put together in anticipation of this day. It was drunk with great delight, I am told.
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One of my favourite things was the specially labelled bottle of champagne my colleague, Aidan, put together in anticipation of this day. It was drunk with great delight, I am told.
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One of my favourite things was the specially labelled bottle of champagne my colleague, Aidan, put together in anticipation of this day. It was drunk with great delight, I am told.
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… here is a group of us, probably marking the 10th - 25th people in line, in the morning just before the #Higgs discovery seminar was ready to allow people in for seats. I met some people that night I’d never met before, but whose paths I then crossed for many years after. I also reconnected with some old colleagues in line that night and morning. It was an electric experience.
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… here is a group of us, probably marking the 10th - 25th people in line, in the morning just before the #Higgs discovery seminar was ready to allow people in for seats. I met some people that night I’d never met before, but whose paths I then crossed for many years after. I also reconnected with some old colleagues in line that night and morning. It was an electric experience.
