global-phase
Differences
This shows you the differences between two versions of the page.
| Both sides previous revisionPrevious revisionNext revision | Previous revision | ||
| global-phase [May 11, 2026 at 14:02] – yanevskiv | global-phase [May 14, 2026 at 11:38] (current) – external edit 127.0.0.1 | ||
|---|---|---|---|
| Line 1: | Line 1: | ||
| + | # Global phase | ||
| + | **Global phase** is a property of a quantum state that comes out of mathematics description of a quantum state. However it is physically completely unobservable and we often ignore it. | ||
| + | |||
| + | |||
| + | To gain an intuition what global phase looks like, let us start from a single qubit written using Dirac notation. Probability amplitudes $a\in\mathbb{C}$ and $b\in\mathbb{C}$ are complex numbers which are respectively associated with the states $\lvert 0\rangle$ and $\lvert 1\rangle$. According to the Born rule, their modulus squared $|a|^2$ and $|b|^2$ are the real probabilities the qubit would collapse to either state $\lvert 0\rangle$ or $\lvert 1\rangle$ | ||
| + | |||
| + | $$\lvert\psi\rangle = a\lvert 0\rangle + b\lvert 1\rangle$$ | ||
| + | |||
| + | Because $a$ and $b$ are complex numbers, we can rewrite them as $Ae^{i\alpha}$ and $Be^{i\beta}$ respectively $A, B\in\mathbb{R}$ and $\alpha, | ||
| + | |||
| + | $$\lvert\psi\rangle = Ae^{i\alpha}\lvert 0\rangle + Be^{i\beta}\lvert 1\rangle$$ | ||
| + | |||
| + | What would happen if created a new qubit $\lvert\psi' | ||
| + | |||
| + | $$\lvert\psi' | ||
| + | |||
| + | It looks like both probability amplitudes accrued the same phase $\phi$. So are qubits $\lvert\psi\rangle$ and $\lvert\psi' | ||
| + | |||
| + | $$\lvert\psi\rangle \sim e^{i\phi}\lvert\psi\rangle$$ | ||
| + | |||
| + | Because global phase is unobservable, | ||
| + | |||
| + | $$\lvert\psi\rangle = e^{i\alpha}\left(A\lvert 0\rangle + Be^{i(\beta - \alpha)}\lvert 1\rangle\right)$$ | ||
| + | |||
| + | Here we can identify $\lvert\psi\rangle \sim e^{i\alpha}\lvert\psi\rangle$ and let $\varphi = \beta - \alpha$ be the relative phase between probability amplitudes. Unlike global phase, relative phase is actually important for entanglement. | ||
| + | |||
| + | $$\lvert\psi\rangle = A\lvert 0\rangle + Be^{i\var}\lvert 1\rangle$$ | ||
| + | |||
| + | ### No change in probabilities | ||
| + | |||
| + | First let's focus on $\lvert\psi\rangle$. | ||
| + | |||
| + | $$\lvert\psi\rangle = Ae^{i\alpha}\lvert 0\rangle + Be^{i\beta}\lvert 1\rangle$$ | ||
| + | |||
| + | Let's apply the Born's rule. Only thing to remember is that $|e^{ix}| = 1$ because it represents a complex number on the unit circle. | ||
| + | |||
| + | $$P_0 = |a|^2 = |Ae^{i\alpha}|^2 = |A|^2|e^{i\alpha}|^2 = |A|^2\cdot 1 = |A|^2 $$ | ||
| + | $$P_1 = |b|^2 = |Be^{i\beta}|^2 = |B|^2|e^{i\beta}|^2 = |B|^2\cdot 1 = |B|^2 $$ | ||
| + | |||
| + | Now let's turn to $\lvert\psi' | ||
| + | $$\lvert\psi' | ||
| + | |||
| + | From this, we can tell that both probability amplitudes accrued a phase shift $\varphi$. This is the global phase. | ||
| + | |||
| + | $$Ae^{i\alpha}\rightarrow Ae^{i(\alpha + \varphi)}$$ | ||
| + | $$Be^{i\beta}\rightarrow Be^{i(\beta + \varphi)}$$ | ||
| + | |||
| + | So now let's reapply Born rule | ||
| + | $$P_0 = |Ae^{i(\alpha + \varphi)}|^2 = |A|^2|e^{i(\alpha + \varphi)}|^2 = |A|^2\cdot 1 = |A|^2 $$ | ||
| + | $$P_1 = |Be^{i(\beta + \varphi)}|^2 = |B|^2|e^{i(\beta + \varphi)}|^2 = |B|^2\cdot 1 = |B|^2 $$ | ||
| + | |||
| + | The probabilities are identical | ||
| + | |||
| + | ### Removing global phase | ||
| + | At this point, we can factor out either $e^{i\alpha}$ or $e^{i\beta}$ let's do the former. | ||
| + | |||
| + | |||
| + | |||
