The square root produces branch points at z=±1, with local behaviour proportional to (z∓1)−1/2. One branch cut can join them along [−1,1]. Another choice uses the two rays (−∞,−1]∪[1,∞). Each choice prevents a loop from enclosing just one branch point within a single-valued domain. For the finite-segment choice fix z2−1∼z at infinity. Infinity is then a pole of order three, not a branch point, since
f(z)=z3+21z+8z3+O(z−3).
Ancestors (12)
- c
- 3
- S1
- 2019
- Past exam of the short options paper shared by Parts A and B of the physics course of the University of Oxford
- Short options paper shared by Parts A and B of the physics course of the University of Oxford
- Physics course of the University of Oxford
- Undergraduate course of the University of Oxford
- Course of the University of Oxford
- University of Oxford
- List of universities
- Home
Discussion (0)
New discussionThere are no discussions about this article yet.
Articles by others on the same topic (0)
There are currently no matching articles.