Anticommutativity of Wedge Product .... Tu, Proposition 3.21

In summary, the sign of a permutation can be decomposed into the product of the signs of its disjoint cycles, which allows us to rewrite the sum in the proof of Proposition 3.21.
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I am reading Loring W.Tu's book: "An Introduction to Manifolds" (Second Edition) ...

I need help in order to fully understand Tu's Proposition 3.21 ... ...

Proposition 3.21 reads as follows:
?temp_hash=c2774c2ad79343dd31fd8b4065264395.png

?temp_hash=c2774c2ad79343dd31fd8b4065264395.png


In the above proof by Tu we read the following:

" ... ...

... ##= \sum_{ \sigma_{ k + l } } ( \text{ sgn } \sigma ) f( v_{ \sigma \tau (l+1) }, \cdot \cdot \cdot , v_{ \sigma \tau (l+k) }) g ( v_{ \sigma \tau (1) }, \cdot \cdot \cdot , v_{ \sigma \tau (l) })####= ( \text{ sgn } \tau ) \sum_{ \sigma_{ k + l } } ( \text{ sgn } \sigma \tau ) g ( v_{ \sigma \tau (1) }, \cdot \cdot \cdot , v_{ \sigma \tau (l) }) f( v_{ \sigma \tau (l+1) }, \cdot \cdot \cdot , v_{ \sigma \tau (l+k) })##

... ... ... "
Can someone please explain/demonstrate how/why we have that##\sum_{ \sigma_{ k + l } } ( \text{ sgn } \sigma ) f( v_{ \sigma \tau (l+1) }, \cdot \cdot \cdot , v_{ \sigma \tau (l+k) }) g ( v_{ \sigma \tau (1) }, \cdot \cdot \cdot , v_{ \sigma \tau (l) })####= ( \text{ sgn } \tau ) \sum_{ \sigma_{ k + l } } ( \text{ sgn } \sigma \tau ) g ( v_{ \sigma \tau (1) }, \cdot \cdot \cdot , v_{ \sigma \tau (l) }) f( v_{ \sigma \tau (l+1) }, \cdot \cdot \cdot , v_{ \sigma \tau (l+k) })##Help will be much appreciated ... ...

Peter

============================================================================

*** EDIT ***I have been reflecting on my question/problem in the above post ... ... and I think I have resolved the problem ...Since ##\text{ sgn } \tau## is ##+1## or ##-1## then ##\text{ sgn } \tau \tau = 1## ...Therefore we have##\text{ sgn } \sigma = \text{ sgn } \sigma \tau \tau = \text{ sgn } \tau \text{ sgn } \sigma \tau##which answers the question ... ...Is that correct ... ... ?

Peter
 

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Yes, that is correct. Well done! :smile:
 
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Yes, your explanation is correct. The sign of a permutation is equal to the product of the signs of its disjoint cycles. Since ##\tau## is a permutation of length ##l + k##, it can be decomposed into disjoint cycles of lengths ##l## and ##k##. Therefore, the sign of ##\tau## is equal to the product of the signs of these cycles, which is equal to ##\text{sgn } \tau \text{ sgn } \sigma \tau##. This is why we can rewrite the sum in the proof as ##( \text{ sgn } \tau ) \sum_{ \sigma_{ k + l } } ( \text{ sgn } \sigma \tau ) g ( v_{ \sigma \tau (1) }, \cdot \cdot \cdot , v_{ \sigma \tau (l) }) f( v_{ \sigma \tau (l+1) }, \cdot \cdot \cdot , v_{ \sigma \tau (l+k) })##.
 

1. What is the Anticommutativity of Wedge Product?

The Anticommutativity of Wedge Product is a mathematical property of the wedge product operation, which is a type of multiplication used in differential geometry and algebraic topology. It states that when two elements are multiplied using the wedge product, the order of the elements does not affect the result. In other words, the product of x and y is the same as the product of y and x.

2. How does Proposition 3.21 in Tu's book relate to the Anticommutativity of Wedge Product?

Proposition 3.21 in Tu's book is a proof of the Anticommutativity of Wedge Product. It shows that for any two elements x and y, their wedge product is equal to the negative of their reverse wedge product. This is a key property in differential geometry and is used in various calculations and proofs.

3. Why is the Anticommutativity of Wedge Product important in mathematics?

The Anticommutativity of Wedge Product is important because it allows for easier manipulation and calculation of geometric and topological objects. It also has applications in physics, such as in the study of vector fields and differential forms. Additionally, it is a fundamental property of the wedge product and is used in various theorems and proofs in mathematics.

4. Can you provide an example of the Anticommutativity of Wedge Product?

Yes, for example, if we have two vectors u and v, their wedge product is denoted as u ∧ v. The Anticommutativity of Wedge Product states that u ∧ v = -v ∧ u. This means that the product of u and v is equal to the negative of the product of v and u. This can also be extended to higher dimensions and more complex objects.

5. Is the Anticommutativity of Wedge Product the same as the Commutativity property?

No, the Anticommutativity of Wedge Product and the Commutativity property are not the same. Commutativity states that the order of elements does not affect the result of a multiplication, while Anticommutativity specifically refers to the wedge product operation and its property of reversing the order of elements. In other words, all wedge products are commutative, but not all mathematical operations are commutative.

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