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Quantum Physics Basics: Double Slit, Superposition and Measurement

Tiny things like photons and electrons are "quantum objects". Each one is detected as a single dot (like a particle), but where the dots land follows a wave of probability, which makes stripes. Before we measure, a quantum object can be in a superposition of possibilities. If we find out which path it took, the stripes disappear. Quantum computers and quantum cryptography use these rules.

🎬 Step-by-step story

  1. Here is a lab: a source of tiny particles (photons or electrons), a wall with two narrow slits, and a screen.
  2. We send ONE particle at a time. Each one lands as one single dot. We cannot say in advance where it will land.
  3. After thousands of dots, a pattern appears: bright and dark stripes. Stripes come from waves, so each particle "went through both slits" as a wave.
  4. The red curve is the probability wave. Where it is high, dots land often. Where it is zero, no dot ever lands.
  5. Now a detector finds out which slit each particle used. The stripes vanish and we see just two bands. Measuring changed the result.
  6. Free play: send single particles or 200 at once, switch the detector on and off, and compare the patterns.

Tip: drag the 3D scene to turn it. Use two fingers to zoom.

🤔 Common doubts, cleared

If each particle makes one dot, where does the wave come in?

In the pattern. One dot shows the particle side; the stripes made by thousands of dots show the wave side.

Can we predict where the next particle will land?

No, only the chances. Each dot is random; the curve tells which places are likely.

Why is there no dot at a dark stripe at all?

The probability waves from the two slits cancel there, so |ψ|² = 0.

Why does watching the slits remove the stripes?

Recording the path ends the superposition of "slit A and slit B", so there is nothing left to interfere.

Do I need to read the detector for the stripes to vanish?

No. If the path information exists anywhere, the stripes vanish. Try switching the detector on in free play.

What is a quantum object?

A quantum object is a very small thing, like a photon (a tiny packet of light) or an electron. It is not a tiny ball and not a water wave. It is something new.

The double-slit experiment, one particle at a time

Shine very weak light at two narrow slits, so weak that only one photon is in the lab at a time. A sensitive screen records each photon as one dot.

  1. The first dots look random.
  2. After thousands of dots, bright and dark stripes (an interference pattern) appear.
  3. Close one slit and the stripes disappear.

So each single photon is affected by both slits. The same happens with electrons, atoms and even big molecules. An interferometer (a device that splits a beam into two paths and joins them again) shows the same thing with single photons.

Try it

In the 3D lab, press "Send 1" ten times. Can you guess where the next dot will land? Then press "+200" several times and watch stripes grow.

Probability waves and the wave function

Physicists describe a quantum object with a wave function, written ψ (psi). It is not a wave of water or air. It is a wave of chances.

Rule (Born rule): the chance of finding the particle at a place is proportional to |ψ|², the square of the wave's size there.

At a dark stripe, the waves from the two slits cancel, so |ψ|² = 0 and no dot ever lands. At a bright stripe they add up, so dots land often.

Superposition and measurement

Superposition means a quantum object can be in a mix of possibilities at once, such as "path A and path B", until it is measured.

Measurement gives one definite answer. After it, the superposition is gone (we say the state "collapses").

Heisenberg uncertainty relation

You cannot know both the exact position and the exact momentum of a quantum object at the same time. In symbols: Δx · Δp ≥ h / 4π, where h = 6.63 × 10⁻³⁴ J s.

Make the slit narrower (smaller Δx) and the particles spread out more after it (bigger Δp). This is not because our tools are bad. It is how nature is.

Quantum technology: qubits, computers and cryptography

A normal bit is 0 or 1. A qubit can be in a superposition of 0 and 1. Measuring it gives 0 or 1 with set chances.

Key formulas and definitions

Worked examples

1. Find the energy of one photon of green light, f = 6.0 × 10¹⁴ Hz.

E = h f = 6.63 × 10⁻³⁴ × 6.0 × 10¹⁴ = 3.98 × 10⁻¹⁹ J (about 2.5 eV).

2. An electron (m = 9.11 × 10⁻³¹ kg) moves at 2.0 × 10⁶ m/s. Find its de Broglie wavelength.

p = m v = 9.11 × 10⁻³¹ × 2.0 × 10⁶ = 1.82 × 10⁻²⁴ kg m/s. λ = h / p = 6.63 × 10⁻³⁴ / 1.82 × 10⁻²⁴ = 3.6 × 10⁻¹⁰ m = 0.36 nm, about the size of an atom.

3. Electrons with λ = 0.36 nm pass two slits d = 1.0 μm apart. The screen is L = 1.0 m away. Find the fringe spacing.

Δy = λ L / d = 0.36 × 10⁻⁹ × 1.0 / 1.0 × 10⁻⁶ = 3.6 × 10⁻⁴ m = 0.36 mm.

4. An electron is known to be inside a region Δx = 1.0 × 10⁻¹⁰ m. Find the smallest uncertainty in its momentum.

Δp ≥ h / (4π Δx) = 6.63 × 10⁻³⁴ / (12.57 × 1.0 × 10⁻¹⁰) = 5.3 × 10⁻²⁵ kg m/s.

5. At a point on the screen, the wave from slit 1 has size 1 and from slit 2 has size 1. Compare the chance there when the waves are in step and when they are opposite.

In step: ψ = 1 + 1 = 2, |ψ|² = 4. Opposite: ψ = 1 − 1 = 0, |ψ|² = 0. So bright stripe (4 times one slit alone) versus dark stripe (no dots).

6. A qubit has a 36% chance of giving 1. It is measured 500 times (fresh each time). About how many 1s do you expect?

0.36 × 500 = 180 ones (and about 320 zeros). Each single result is random; only the count is predictable.

Common mistakes

Practice quiz

1. When single photons hit the screen one by one, each one makes:
2. After thousands of single photons, the screen shows:
3. The chance of finding a particle at a point depends on:
4. If a detector records which slit each electron uses, the stripes:
5. A qubit, before measurement, can be:

Practice: answer these yourself

Type or choose your answer, then press Check. Use a hint if you are stuck; the full solution appears after you answer.

Frequently asked questions

Does the particle really go through both slits?

Its probability wave goes through both slits and interferes. When we detect the particle, it is found in one place. Asking "which slit?" without measuring has no definite answer.

Why don't we see quantum effects with cricket balls?

A ball's de Broglie wavelength is far too tiny to see, and decoherence (constant bumping with air and light) destroys its superposition almost instantly.

Is quantum physics used in daily life?

Yes: transistors in phones, lasers, LEDs, solar cells, MRI scanners and GPS atomic clocks all rely on quantum rules.

Where this is taught

South Korea고등학교 2학년Quantum and the micro world
Germany (Bavaria)Jahrgangsstufe 13Basic ideas of quantum physics

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