Consider any one-dimensional wave function describing a quantum mechanical particle. The value of the wave function at point is , at point is , and so on.[1]
Then, we can represent all the function values as a list; we can then take this column vector that lives in an abstract space and represent it with its elements as follows:
Visualizing in linear algebra
, & could be considered as three different coordinate axes. (You could consider infinitely many elements - but visualizing any more than 3 dimensions geometrically proves difficult.)
Now, can be considered a state vector.
Since there are infinitely possible values, there must also be infinitely many values. And if there are infinite many function values, then the space in which state vector is infinite dimensional; and this abstract space, in which various quantum mechanical vectors live, is called Hilbert Space. Although this is an infinite dimensional vector space, it can also be finite dimensional space.
Hilbert Space with 2 dimensions
The spin up and spin down state which describe a single particle, (both) live in a two-dimensional Hilbert space, which means vectors like have only two components.
Wave function vs State-vector representation
To better distinguish the state-vector representation, of a quantum mechanical particle, from the wave-function representation, we can use the bra-ket notation.
Now, can be represented as a state-vector with or , or as a wave-function with
Bra & Ket Vectors
There are two types of vectors in Dirac notation: the bra vector and the ket vector, named such because when put together they form a braket or an Inner Product.
If is a column vector, then you can write it in Dirac notation as , where the denotes that it's a unit column vector (or a ket vector). The vector adjoined to the ket vector is denoted as is called bra vector.
For a compact notation, we write the bra vector with a inverted arrow : .
Note
or is obtained by applying entry-wise Complex Conjugation to the elements of the transpose of . The bra-ket notation directly implies that is the inner product of vector with itself, which is by definition 1.
Info
More generally, if and are quantum state vectors, then their inner product is . This inner product implies that the probability of measuring the state to be is .
Scalar Product
If and are quantum state vectors, we can represent the dot
Representing the Hadamard operation with Dirac Notation
The following notation is often used to describe the states that result from applying the Hadamard gate to to . These states correspond to the unit vector in the and the directions on the Bloch Sphere: