Basic

量子叠加(superposition)、量子纠缠(entanglement)、量子干涉(interference)

单个 qubit

基态(Deterministic State)

  • ∣0⟩\ket{0}
  • ∣1⟩\ket{1}

∣⟩\ket{} is called a ket.

叠加态(Superposition State)

∣φ⟩=a∣0⟩+b∣1⟩=(ab)\ket{\varphi}=a\ket{0}+b\ket{1}=\begin{pmatrix}a \\ b\end{pmatrix}

表示:对这个 qubit 进行「测量」操作的时候,有 ∣a∣2|a|^2 的概率得到 0,有 ∣b∣2|b|^2 的概率得到 1,其中 ∣a∣2+∣b∣2=1|a|^2+|b|^2=1。

两个常见的叠加态:

  • ∣+⟩=12(∣0⟩+∣1⟩)\ket{+}=\frac{1}{\sqrt{2}}\left(\ket{0}+\ket{1}\right)
  • ∣−⟩=12(∣0⟩−∣1⟩)\ket{-}=\frac{1}{\sqrt{2}}\left(\ket{0}-\ket{1}\right)

其他:

  • ∣±⟩=12(∣0⟩±∣1⟩)\ket{±}=\frac{1}{\sqrt{2}}\left(\ket{0}±\ket{1}\right)
  • ∣0⟩=12(∣+⟩+∣−⟩)\ket{0}=\frac{1}{\sqrt{2}}\left(\ket{+}+\ket{-}\right)
  • ∣1⟩=12(∣+⟩−∣−⟩)\ket{1}=\frac{1}{\sqrt{2}}\left(\ket{+}-\ket{-}\right)
  • ∣μ⟩=12(∣0⟩+i∣1⟩)\ket{\mu}=\frac{1}{\sqrt{2}}\left(\ket{0}+i\ket{1}\right)
  • ∣ν⟩=12(∣0⟩−i∣1⟩)\ket{\nu}=\frac{1}{\sqrt{2}}\left(\ket{0}-i\ket{1}\right)

布洛赫球面(Bloch Sphere)

Bloch Sphere
Bloch Sphere

Qubit state: cos⁡(θ/2)∣0⟩+eiφsin⁡(θ/2)∣1⟩\cos{\left(\theta/2\right)}\ket{0}+e^{i\varphi}\sin{\left(\theta/2\right)}\ket{1}

Polar angle: θ\theta

Azimuthal Angle: φ\varphi

  • ∣0⟩:θ=0,φ=0\ket{0}:\theta=0,\varphi=0
  • ∣1⟩:θ=π,φ=0\ket{1}:\theta=\pi,\varphi=0
  • ∣+⟩:θ=π/2,φ=0\ket{+}:\theta=\pi/2,\varphi=0
  • ∣−⟩:θ=π/2,φ=π\ket{-}:\theta=\pi/2,\varphi=\pi
  • ∣μ⟩:θ=π/2,φ=3π/2\ket{\mu}:\theta=\pi/2,\varphi=3\pi/2
  • ∣ν⟩:θ=π/2,φ=π/2\ket{\nu}:\theta=\pi/2,\varphi=\pi/2

单量子门

  • Hadamard Gate - H
  • Identity Gate - I
  • 非门 - X
  • Z Gate - Z
  • S Gate - S (S=ZS=\sqrt{Z})

Every quantum gate must always be reversible.

H=[111−1],I=[1001],X=[0110],Z=[100−1],S=[100i]H=\begin{bmatrix}1&1\\1&-1\end{bmatrix}, I=\begin{bmatrix}1&0\\0&1\end{bmatrix}, X=\begin{bmatrix}0&1\\1&0\end{bmatrix}, Z=\begin{bmatrix}1&0\\0&-1\end{bmatrix}, S=\begin{bmatrix}1&0\\0&i\end{bmatrix}

  • H∣0⟩=∣+⟩H\ket{0}=\ket{+}, H∣1⟩=∣−⟩H\ket{1}=\ket{-}, H∣+⟩=∣0⟩H\ket{+}=\ket{0}, H∣−⟩=∣1⟩H\ket{-}=\ket{1}
  • H⋅H=IH\cdot H=I
  • I∣0⟩=∣0⟩I\ket{0}=\ket{0}, I∣1⟩=∣1⟩I\ket{1}=\ket{1}, I∣+⟩=∣+⟩I\ket{+}=\ket{+}, I∣−⟩=∣−⟩I\ket{-}=\ket{-}
  • X∣0⟩=∣1⟩X\ket{0}=\ket{1}, X∣1⟩=∣0⟩X\ket{1}=\ket{0}
  • Z∣0⟩=∣0⟩Z\ket{0}=\ket{0}, Z∣1⟩=−∣1⟩Z\ket{1}=-\ket{1}, Z∣+⟩=∣−⟩Z\ket{+}=\ket{-}, Z∣−⟩=∣+⟩Z\ket{-}=\ket{+}
  • S∣+⟩=∣μ⟩S\ket{+}=\ket{\mu}, S∣−⟩=∣ν⟩S\ket{-}=\ket{\nu}

The phase gate S and Z are 90° and 180° rotations around the vertical axis, often referred to as the z-axis.

The quantum NOT gate X is a 180° rotation around the horizontal axis between the Hadamard states, often referred to as the x-axis.

The Hadamard gate H is a 180° rotation around a diagonal between the x and z axes.

Rx(θ)=[cos⁡(θ/2)−isin⁡(θ/2)−isin⁡(θ/2)cos⁡θ/2]R_x(\theta)=\begin{bmatrix} \cos(\theta/2) & -i \sin(\theta/2) \\ -i \sin(\theta/2) & \cos{\theta/2} \end{bmatrix}

Rz(φ)=[100eiφ/2]R_z(\varphi)=\begin{bmatrix} 1 & 0 \\ 0 & e^{i\varphi/2} \end{bmatrix}

Entanglement 纠缠

The Bell state is the prototypical example of an entangled state.

∣φ⟩bell=12(∣00⟩+∣11⟩)\ket{\varphi}_{bell}=\frac{1}{\sqrt{2}}\left(\ket{00}+\ket{11}\right)