kith
Science Advisor
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I would put it like this.
For an abstract vector space V, it is wrong to write expressions like \vec v = (1, 2, 3)^T. The object (1, 2, 3)^T is not itself a vector in V but a representation of such a vector in a certain basis.
But it is straightforward to take tuples like (1, 2, 3)^T and construct a different vector space out of them. This space is called a coordinate space and denoted by K^n. Its elements are tuples so if we are talking about vectors from this space it is fine to write \vec v = (1, 2, 3)^T. Such vectors can again be represented in any basis. This leads to the notation becoming ambiguous: with (1, 2, 3)^T I can either denote a vector or the representation of a vector in a certain basis. (Regarding bases, a coordinate vector space has a special kind of basis: the standard basis \{\vec e_1, ..., \vec e_n\}. It is distinguished by the property that the coefficients of the representations of tuple vectors in this basis are identical to the tuple's components.)
I sometimes use the notation \vec v \doteq (1, 2, 3)^T to denote a certain representation of \vec v, something which I adopted form Sakurai's Modern Quantum Mechanics.
For an abstract vector space V, it is wrong to write expressions like \vec v = (1, 2, 3)^T. The object (1, 2, 3)^T is not itself a vector in V but a representation of such a vector in a certain basis.
But it is straightforward to take tuples like (1, 2, 3)^T and construct a different vector space out of them. This space is called a coordinate space and denoted by K^n. Its elements are tuples so if we are talking about vectors from this space it is fine to write \vec v = (1, 2, 3)^T. Such vectors can again be represented in any basis. This leads to the notation becoming ambiguous: with (1, 2, 3)^T I can either denote a vector or the representation of a vector in a certain basis. (Regarding bases, a coordinate vector space has a special kind of basis: the standard basis \{\vec e_1, ..., \vec e_n\}. It is distinguished by the property that the coefficients of the representations of tuple vectors in this basis are identical to the tuple's components.)
I sometimes use the notation \vec v \doteq (1, 2, 3)^T to denote a certain representation of \vec v, something which I adopted form Sakurai's Modern Quantum Mechanics.