Posting mainly about history of physics.
Too many interesting things to learn, too few time.
Born at 316.91 ppm
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Rodrigues died in relative obscurity, with even the precise date of his death being uncertain. The fact that he was a mathematician was often forgotten by early historians of Saint-Simonism,
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Rodrigues died in relative obscurity, with even the precise date of his death being uncertain. The fact that he was a mathematician was often forgotten by early historians of Saint-Simonism,
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After a long period away from mathematics, Rodrigues published his most significant mathematical work in 1840 on the rotation group. This paper broke from the traditional dynamics-focused approach of Euler to study the geometry of rigid body
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After a long period away from mathematics, Rodrigues published his most significant mathematical work in 1840 on the rotation group. This paper broke from the traditional dynamics-focused approach of Euler to study the geometry of rigid body
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Shifting from academia, Rodrigues followed his family into finance but soon became a devoted disciple and financial supporter of the charismatic utopian socialist Claude-Henri de Saint-Simon. Following Saint-Simon's death, Rodrigues
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Shifting from academia, Rodrigues followed his family into finance but soon became a devoted disciple and financial supporter of the charismatic utopian socialist Claude-Henri de Saint-Simon. Following Saint-Simon's death, Rodrigues
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This formula is his main legacy in modern physics
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This formula is his main legacy in modern physics
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As a Jew, he gained citizenship rights under Napoleon, but the Bourbon restoration in 1815 blocked his path
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As a Jew, he gained citizenship rights under Napoleon, but the Bourbon restoration in 1815 blocked his path
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The formula, based on an assumption that the mass operator is a sum of a dominant SU(3)-invariant term and a symmetry-breaking term, provides a way to calculate the mass of a particle within an SU(3) multiplet...
The formula, based on an assumption that the mass operator is a sum of a dominant SU(3)-invariant term and a symmetry-breaking term, provides a way to calculate the mass of a particle within an SU(3) multiplet...
Thanks.
Thanks.
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The Gell-Mann-Okubo mass formula was part of Gell-Mann's earlier classification scheme known as the Eightfold Way (or SU(3) flavor symmetry).
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The Gell-Mann-Okubo mass formula was part of Gell-Mann's earlier classification scheme known as the Eightfold Way (or SU(3) flavor symmetry).
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The Gell-Mann-Okubo formula:
M(I,Y)=a+bY+c[(1/4)Y²−I(I+1)]
where M is the mass, Y is the hypercharge, I is the isospin, and a, b, and c are constants
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The Gell-Mann-Okubo formula:
M(I,Y)=a+bY+c[(1/4)Y²−I(I+1)]
where M is the mass, Y is the hypercharge, I is the isospin, and a, b, and c are constants
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For the baryon octet, the formula yielded a mass relation that was well-satisfied by existing data. For the baryon decouplet, it predicted an equal mass spacing between members.
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For the baryon octet, the formula yielded a mass relation that was well-satisfied by existing data. For the baryon decouplet, it predicted an equal mass spacing between members.
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Susumu Okubo noted that this approach was awkward for certain baryons.
Okubo's main contribution was providing a successful mass formula for the SU(3) theory.
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Susumu Okubo noted that this approach was awkward for certain baryons.
Okubo's main contribution was providing a successful mass formula for the SU(3) theory.
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People working on the Reductionist Approach proposed that hadrons were bound states of simpler, fundamental objects. Shoichi Sakata's model, for instance, proposed
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People working on the Reductionist Approach proposed that hadrons were bound states of simpler, fundamental objects. Shoichi Sakata's model, for instance, proposed
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In the Nuclear Democracy approach, based on S-matrix theory, all hadrons are considered as equally elementary
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In the Nuclear Democracy approach, based on S-matrix theory, all hadrons are considered as equally elementary
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In the first approach, physicists aimed to find a larger symmetry group containing SU(2)⊗U(1), that would approximately describe strong interactions.
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In the first approach, physicists aimed to find a larger symmetry group containing SU(2)⊗U(1), that would approximately describe strong interactions.
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This led to a larger group, SU(2) ⊗ U(1).
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This led to a larger group, SU(2) ⊗ U(1).
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