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beginner · Physics · Math Foundations: Complex Numbers

Euler’s Formula

One of the most powerful identities in all of mathematics connects the complex exponential to trigonometry. For any real angle θ\theta (in radians),

eiθ=cos⁡θ+isin⁡θ.e^{i\theta} = \cos\theta + i\sin\theta.

This is Euler's formula. It means that the complex exponential eiθe^{i\theta} is a point on the unit circle in the complex plane, at angle θ\theta from the positive real axis. The real part is cos⁡θ\cos\theta and the imaginary part is sin⁡θ\sin\theta, so its modulus is always 1:

∣eiθ∣2=cos⁡2θ+sin⁡2θ=1.|e^{i\theta}|^2 = \cos^2\theta + \sin^2\theta = 1.

The last equality follows from the Pythagorean identity, confirming that eiθe^{i\theta} stays exactly on the unit circle for every θ\theta.

Why it matters for quantum mechanics

A quantum state amplitude is a complex number, and rotating that amplitude by an angle θ\theta multiplies it by eiθe^{i\theta}. Because ∣eiθ∣=1|e^{i\theta}| = 1, this rotation — called a phase — leaves the measurement probability ∣z∣2|z|^2 unchanged. Euler's formula makes this fact transparent: phases are pure rotations on the unit circle. This is why quantum gates like the T gate (rotation by π/4\pi/4) and S gate (rotation by π/2\pi/2) are expressed in terms of eiθe^{i\theta}.

Deriving the formula

A concise route uses Taylor series. Expanding exe^{x}, cos⁡x\cos x, and sin⁡x\sin x around x=0x = 0:

ex=1+x+x22!+x33!+x44!+⋯e^x = 1 + x + \frac{x^2}{2!} + \frac{x^3}{3!} + \frac{x^4}{4!} + \cdots

Substitute x=iθx = i\theta and use i2=−1i^2 = -1, i3=−ii^3 = -i, i4=1i^4 = 1, cycling every four powers:

eiθ=1+iθ−θ22!−iθ33!+θ44!+⋯e^{i\theta} = 1 + i\theta - \frac{\theta^2}{2!} - \frac{i\theta^3}{3!} + \frac{\theta^4}{4!} + \cdots

Separating real and imaginary parts:

eiθ=(1−θ22!+θ44!−⋯ )+i(θ−θ33!+θ55!−⋯ )=cos⁡θ+isin⁡θ.e^{i\theta} = \left(1 - \frac{\theta^2}{2!} + \frac{\theta^4}{4!} - \cdots\right) + i\left(\theta - \frac{\theta^3}{3!} + \frac{\theta^5}{5!} - \cdots\right) = \cos\theta + i\sin\theta.

The two bracket expressions are exactly the Taylor series for cos⁡θ\cos\theta and sin⁡θ\sin\theta, completing the derivation.

Special values

Several angles give exact results worth memorizing:

| θ\theta | eiθe^{i\theta} | |---|---| | 00 | 11 | | π/6\pi/6 | 32+i2\dfrac{\sqrt{3}}{2} + \dfrac{i}{2} | | π/4\pi/4 | 12+i2\dfrac{1}{\sqrt{2}} + \dfrac{i}{\sqrt{2}} | | π/3\pi/3 | 12+i32\dfrac{1}{2} + \dfrac{i\sqrt{3}}{2} | | π/2\pi/2 | ii | | π\pi | −1-1 | | 2π2\pi | 11 |

The case θ=π\theta = \pi gives eiπ=−1e^{i\pi} = -1, or equivalently eiπ+1=0e^{i\pi} + 1 = 0 — often called Euler's identity.

Try it

This is a numerical exercise — your code should return a number. Using Euler's formula, eiθ=cos⁡θ+isin⁡θe^{i\theta} = \cos\theta + i\sin\theta, find the real part of eiπ/3e^{i\pi/3}.

From the table above (and the 30-60-90 triangle), cos⁡(π/3)=1/2=0.5\cos(\pi/3) = 1/2 = 0.5 exactly.

Run your code to see the quantum state.

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