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Art of Spin Decomposition Xiang-Song Chen 陈陈陈 Huazhong Univ. of Sci. & Tech. 陈陈陈陈陈陈 Outline: Spin sum rules and controversies A most familiar example What makes a good spin decomposition Angular momentum of tensor gauge field Critical thinking about gauge invariance

Art of Spin Decomposition

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Art of Spin Decomposition. Outline: Spin sum rules and controversies A most familiar example What makes a good spin decomposition Angular momentum of tensor gauge field Critical thinking about gauge invariance. Xiang-Song Chen 陈相松 Huazhong Univ. of Sci. & Tech. 华中科技大学. - PowerPoint PPT Presentation

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Page 1: Art of Spin Decomposition

Art of Spin Decomposition

Xiang-Song Chen 陈相松Huazhong Univ. of Sci. & Tech. 华中科技大学

Outline:

Spin sum rules and controversies

A most familiar example

What makes a good spin decomposition

Angular momentum of tensor gauge field

Critical thinking about gauge invariance

Page 2: Art of Spin Decomposition

Related recent papers1) Art of spin decomposition Xiang-Song Chen, Wei-Min Sun, Fan Wang, T. Goldman, Phys. Rev. D 83, 071901(R) (2011).

2) Proper identification of the gluon spin Xiang-Song Chen, Wei-Min Sun, Fan Wang, T. Goldman, Phys. Lett. B 700, 21 (2011).

3) Physical decomposition of the gauge and gravitational fields Xiang-Song Chen, Ben-Chao Zhu, Phys. Rev. D 83, 084006 (2011).

4) Spin and orbital angular momentum of the tensor gauge field. Xiang-Song Chen, Ben-Chao Zhu, Niall Ó Murchadha, arXiv:1105.6300v1

5) Tensor gauge condition and tensor field decomposition Xiang-Song Chen, Ben-Chao Zhu, arXiv:1101.2809v4

Page 3: Art of Spin Decomposition

3 3 3 3

3 3

total

3total

Jaffe-Manohar [NPB337, 509 (1990)]

Ji [PRL78, 610 (1997)], Chen-Wang [CTP27, 212 (1997)

1

]

Chen-L

1

2

1 1

2

i id x d x E Ax d x d x

d x d x d x

x E Ai

x D x E Bi

J

J

3 3 3total

tota

3pure phys pure p y

l3

h s

u-Sun-Wang-Goldman [PRL100,232002 (2008); 103,062001 (2009)]

Wakamatsu [PRD81, 114010(2010); arXiv:1007.5355

1 1D

2

]

1

2

i id x d x d x dx D E A x E Ax

d

i

x

J

J

total

phys pure phys phys

pure phys pure p

3 3 3

ys3 3

h3 3

Cho-Ge-Zhang [arXiv:1010.1080

1( D )

1D

]

1

2

i i a a

iR D iC

x D E A x E A Ai

x D E A x E

d x d x d x

d x d x d x d xJ Ai

Earlier and recent Spin sum rules

Page 4: Art of Spin Decomposition

A most familiar example: Solving the hydrogen atom

Does this make sense???

Page 5: Art of Spin Decomposition

The atom as a whole

Page 6: Art of Spin Decomposition

Close look at the photon contribution

The static terms!

Page 7: Art of Spin Decomposition

Justification of neglecting photon field

Page 8: Art of Spin Decomposition

A critical gap to be closed

Page 9: Art of Spin Decomposition

The same story with Hamiltonian

Page 10: Art of Spin Decomposition

The fortune of using Coulomb gauge

Page 11: Art of Spin Decomposition

Momentum of a moving atom

A stationary electromagnetic field carries no momentum

Page 12: Art of Spin Decomposition

Gauge-invariant revision

Page 13: Art of Spin Decomposition

The covariant scheme

spurious photon angular momentum

Page 14: Art of Spin Decomposition

Gluon angular momentum in the nucleon:

Tree-level

0

)( ' 3

BErxdJ g

One-gluon exchange has the same property as

one-photon exchange

Page 15: Art of Spin Decomposition

Beyond the static approximation

Page 16: Art of Spin Decomposition

The tensor gauge field

Page 17: Art of Spin Decomposition

Canonical expression of spin and OAM

Page 18: Art of Spin Decomposition

Canonical expression of spin and OAM

Page 19: Art of Spin Decomposition

Complete tensor gauge conditions

Page 20: Art of Spin Decomposition

Vanishing of angular momentum for a stationary tensor gauge field

No spurious time-

dependence

Page 21: Art of Spin Decomposition

The same property of momentum

Page 22: Art of Spin Decomposition

Critical thinking about gauge invariance: Gauge theory as a “Compromising” Physical Theory

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)

Conditions Results

Page 23: Art of Spin Decomposition

Gauge invariance: “The emperor’s new clothes”?

This clothes is made of

QCD vacuum. Intelligent

people see a splendid

structure. Stupid people see nothing!

Selling for one million dollars!

Wonderful! I buy it.

Great! We have

produced GDP of one million

dollars!

Page 24: Art of Spin Decomposition

Demonstration with a key issue:Quantum Lorentz Invariance with

Tensor Gauge Coupling

Lorentz Invariance of Quantum Gravity

Page 25: Art of Spin Decomposition

Two keywords in modern physics

• Quantization (量子化 )

• Symmetry (对称性 ) 1) Space-time symmetry

2) Gauge symmetry

Page 26: Art of Spin Decomposition

Classical Lorentz Invariance

Four-vector gauge field

Page 27: Art of Spin Decomposition

Quantum Lorentz Invariance

Page 28: Art of Spin Decomposition

Clarification on Lorentz Covariance

1 1T. Goldman et al.: using (1,0) (0,1) instead of ( , )

2 2

Page 29: Art of Spin Decomposition

Two approaches towards quantum Lorentz Invariance in gauge theory

• Covariant quantization with non-physical states

• Physical quantization with non-covariant propagator

Page 30: Art of Spin Decomposition

Electrodynamics: vector gauge coupling

• Covariant quantization with non-physical states: Gupta-Bleuler

• Physical quantization with non-covariant propagator: Coulomb gauge

Page 31: Art of Spin Decomposition

The non-covariant propagator of Physical photon

Page 32: Art of Spin Decomposition

A delicate point: the contact term and its effect

Page 33: Art of Spin Decomposition

Cancelation of the contact term

Page 34: Art of Spin Decomposition

The fortune of Abelian gauge theory: Uniqueness of Coulomb gauge

Page 35: Art of Spin Decomposition

Gravitation as tensor gauge coupling

Page 36: Art of Spin Decomposition

The physical graviton propagator

Page 37: Art of Spin Decomposition

Propagator of general gauge field

Page 38: Art of Spin Decomposition

The contact term and its effect

Page 39: Art of Spin Decomposition

Choice of tensor gauge conditions: Non-uniqueness

Page 40: Art of Spin Decomposition

Hamiltonian in various gauges

Test for Quantum Lorentz Invariance!

Page 41: Art of Spin Decomposition

Thank you!谢谢 !