$ \newcommand{\braket}[1]{\langle #1 \rangle} \newcommand{\abs}[2][]{\left\lvert#2\right\rvert_{\text{#1}}} \newcommand{\ket}[1]{\left\lvert#1 \right.\rangle} \newcommand{\bra}[1]{\langle\left. #1\right\rvert} \newcommand{\braket}[1]{\langle #1 \rangle} \newcommand{\dd}{\text{d}} \newcommand{\dv}[2]{\frac{\dd #1}{\dd #2}} \newcommand{\pdv}[2]{\frac{\partial}{\partial #1}} $
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Overview
Notations
Concepts
a ket is used to represent a quantum system. A bra is the conjungate vector.
They're members of the Hilbert space

Notations

It's basically just the physics notation for column and row vectors

Concepts

The bra is the conjungate transpose of a ket. To turn a ket int a bra, you need to take the complex conjungate of each term.
a ket is used to represent a quantum system. A bra is the conjungate vector.
They're members of the Hilbert space

Notations

It's basically just the physics notation for column and row vectors

Concepts

The bra is the conjungate transpose of a ket. To turn a ket int a bra, you need to take the complex conjungate of each term.
FullPage
Overview
Notations
Concepts
FullPage
Overview
Notations
Concepts
a ket is used to represent a quantum system. A bra is the conjungate vector.
They're members of the Hilbert space

Notations

It's basically just the physics notation for column and row vectors

Concepts

The bra is the conjungate transpose of a ket. To turn a ket int a bra, you need to take the complex conjungate of each term.
a ket is used to represent a quantum system. A bra is the conjungate vector.
They're members of the Hilbert space

Notations

It's basically just the physics notation for column and row vectors

Concepts

The bra is the conjungate transpose of a ket. To turn a ket int a bra, you need to take the complex conjungate of each term.
FullPage
Overview
Notations
Concepts