Two questions on linear transformations.

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The discussion centers on two questions regarding the linearity of transformations defined over complex and real fields. For the first question, it is noted that if a transformation f: C^n -> C^n is linear over R with a rank of 3, it cannot be linear over C due to dimensionality constraints, as C^n is a 2n-dimensional real vector space. In the second question, a function f: C -> C that is linear over R with a negative determinant suggests it is invertible over R, but its linearity over C remains uncertain. Participants express confusion regarding the interpretation of linearity and dimensionality in the context of complex vector spaces. The conversation highlights the need for clarity in defining linearity in relation to the fields involved.
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1) there's given a transformation f:C^n->C^n (C is the complex field), it's known that f is linear on R (real numbers) and its rank on R equals 3 i.e, dim_R Imf=3. now is f linear on C?
2) there's a function f:C->C and its known that f is linear on R, and det_R f<0, is f linear on C?

im kind of stuck on those questions, obviously in the second question, if the determinant is different than zero then the matrix is invertible (i.e has an inverse) and so it has an f^-1, so it's isomorphism on R, but I am not sure if its linear on C.

now about the first question if dim_R Imf=3<n then function isn't onto C^n and thus isn't injective, but i don't know how to deduce from that about its linearity on C.

your help is apprecited.
 
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loop quantum gravity said:
1) there's given a transformation f:C^n->C^n (C is the complex field), it's known that f is linear on R (real numbers) and its rank on R equals 3 i.e, dim_R Imf=3. now is f linear on C?
2) there's a function f:C->C and its known that f is linear on R, and det_R f<0, is f linear on C?

im kind of stuck on those questions, obviously in the second question, if the determinant is different than zero then the matrix is invertible (i.e has an inverse) and so it has an f^-1, so it's isomorphism on R, but I am not sure if its linear on C.

now about the first question if dim_R Imf=3<n then function isn't onto C^n and thus isn't injective, but i don't know how to deduce from that about its linearity on C.

your help is apprecited.

I am confused by this. If f is defined on Cn, what do you mean by "f is linear on R"? Do you mean on (x+ 0i,0,0...)? And it has to have rank 3? How can a function defined on a one-dimensional vector space have rank 3?
 
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i think it means:
for example, that the basis of C^n is (1,0,...,0),...(0,0,...0,1),(i,0,...,0),...(0,...,i)
where on C it would only be the first n vectors.
 
Hmm. There are several ways to interpret this question.

R^n is an obvious real subspace of C^n, but that is an artificial way of thinking about things - and the canonical counter example is to take the transformation that conjugates in each variable.

No, you really have to think about this as C^n being a 2n dimensional real vector space.

Anyway, buried in there is the hint: as a real vector space, C^m is 2m dimensional, and the image of f is a complex vector space, so it certainly can't be a 3 dimensional real vector space, can it?
 
loop quantum gravity said:
i think it means:
for example, that the basis of C^n is (1,0,...,0),...(0,0,...0,1),(i,0,...,0),...(0,...,i)
where on C it would only be the first n vectors.
No, a basis for C^n is (1, 0, ...,0)... (0, 0, ..., 1). Since you are multiplying by complex numbers. Do you mean to say a basis for C^n as a vector space over R?

matt, my problem is that the problem did not say "linear on R^n", it said "linear on R". Exactly how are you thinking of a function from C^n to C^n as restricted to R?
 
I was taking 'linear on R' to mean R-linear (linear *over* R), the normal meaning we'd take for field extensions K over k, which is almost certainly what should have been written.
 
I am studying the mathematical formalism behind non-commutative geometry approach to quantum gravity. I was reading about Hopf algebras and their Drinfeld twist with a specific example of the Moyal-Weyl twist defined as F=exp(-iλ/2θ^(μν)∂_μ⊗∂_ν) where λ is a constant parametar and θ antisymmetric constant tensor. {∂_μ} is the basis of the tangent vector space over the underlying spacetime Now, from my understanding the enveloping algebra which appears in the definition of the Hopf algebra...

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