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Towards a final criteria of separating momentum and angular momentum Outline: I.The matter of convenience II.The matter of reasonableness III.The matter of correctness Xiang-Song Chen Huazhong University of Science & Technology 陈相松 华中科技大学 武汉 16 Feb 2012 @ INT-Seattle
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Recall of the Controversies Leader [PRD 83:096012 (2011)]
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Hint from a forgotten practice: Why photon is ignored for atomic spin? The fortune of choosing Coulomb gauge Quantitative differences Fine-tuning for the gluon spin and OAM I. The matter of convenience and fine-tuning in actual application
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Hint from a forgotten practice: Why photon is ignored for atomic spin? Do these solutions make sense?!
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The atom as a whole
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Close look at the photon contribution The static terms!
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Justification of neglecting photon field
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A critical gap to be closed
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The same story with Hamiltonian
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The fortune of using Coulomb gauge
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Momentum of a moving atom A stationary electromagnetic field carries no momentum
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Gauge-invariant revision – Angular Momentum
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Gauge-invariant revision -Momentum and Hamiltonian
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The covariant scheme spurious photon angular momentum
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Gluon angular momentum in the nucleon: Tree-level One-gluon exchange has the same property as one-photon exchange
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Beyond the static approximation
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Fine-tuning for the gluon spin and OAM Possible convergence in evolution
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Leader’s compelling criteria to remove the controversy Recalling the Poincare algebra and subalgebra for and interacting system Generators for the physical fields: QED The quark-gluon system II. The matter of reasonableness ---Leader’s criteria of separating momentum and angular momentum
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The controversy and Leader’s Criteria
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Interacting theory: Structure of Poincare generators
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Interacting theory: Poincare (sub)algebra
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Generators for the gauge-invariant physical fields - translation
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Generators for the gauge-invariant physical fields - Rotation
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The quark-gluon system
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Generator for the gauge- invariant quark field
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Generator for the gauge- invariant gluon field
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Some detail in the proof
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III. Possibly a real final solution Dipole rad. (rad. gauge) l=1 m=1 E Flux J Flux
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Miracle of quantum Measurement A system can only be detected in certain eigenstate E.g. Optical pumping of a trapped ion
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The issue of “indirect” observable in QCD: matter of definition, but … The same experiments as to “measure” the conventional PDFs New factorization formulae and extraction of the new PDFs Quark and gluon orbital angular momentum can in principle be measured through generalized (off- forward) PDFs
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Is gauge-invariance a “Compromise”, or even “illusion”? First step in Physics : Complete Description Classic Physics: r and p ( controllable ) Quantum Mechanics : Wave Function ( Not completely controllable ) Gauge Theory : Gauge potentials (Completely uncontrollable ) Need for the physical variable: Real emergence of a photon
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Thank you! 谢谢 !
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