Understanding Spinor Rotations

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SUMMARY

The discussion centers on the behavior of spinors under rotations, specifically addressing the spin rotation matrix and its effect on spinor components. The spin rotation matrix is defined as U = \left( \begin{array}{ccc} e^{-\frac{i}{2}\phi} & 0 \\ 0 & e^{\frac{i}{2}\phi} \end{array} \right). A 2π rotation results in the transformation \xi ' = \left( \begin{array}{ccc} e^{-i\pi} & 0 \\ 0 & e^{i\pi} \end{array} \right) \left( \begin{array}{c} \xi_{1} \\ \xi_{2} \end{array} \right) = (-\xi_{1}, \xi_{2}), indicating that only one component of the spinor changes sign. This confirms that the transformation leads to \hat{U} \xi = -\xi, validating the behavior of spinors under such rotations.

PREREQUISITES
  • Understanding of spinor mathematics
  • Familiarity with quantum mechanics concepts
  • Knowledge of rotation matrices
  • Basic grasp of complex exponentials
NEXT STEPS
  • Study the properties of spinors in quantum mechanics
  • Learn about the implications of SU(2) representations
  • Explore the mathematical framework of rotation matrices in higher dimensions
  • Investigate the significance of the 2π rotation in quantum systems
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Physicists, mathematicians, and students studying quantum mechanics, particularly those interested in the behavior of spinors and their transformations under rotations.

gentsagree
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Hi,

I am confused on a very basic fact. I can write \xi = (\xi_{1}, \xi_{2}) and a spin rotation matrix as

<br /> U =<br /> \left( \begin{array}{ccc}<br /> e^{-\frac{i}{2}\phi} &amp; 0 \\<br /> 0 &amp; e^{\frac{i}{2}\phi} <br /> \end{array} \right)<br />

A spinor rotates under a 2\pi rotation as

<br /> \xi &#039; = <br /> \left( \begin{array}{ccc}<br /> e^{-i\pi} &amp; 0 \\<br /> 0 &amp; e^{i\pi} <br /> \end{array} \right)<br /> \left( \begin{array}{c}<br /> \xi_{1} \\<br /> \xi_{2}<br /> \end{array} \right)<br /> =<br /> \left( \begin{array}{ccc}<br /> -\xi_{1} \\<br /> \xi_{2} <br /> \end{array} \right)<br />

which is (-\xi_{1}, \xi_{2}), and not -\xi, so only one component changes sign. Is this correct?
 
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How do you come to this conclusion? Since ##\exp(\mathrm{i} \pi)=\exp(-\mathrm{i} \pi)=-1## your rotation by ##2 \pi## leads to ##\hat{U} \xi=-\xi## as it should be.
 
Ahah, ok, I should not try to do physics today.
 

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