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๐Ÿš€ ๐Ÿฏ๐Ÿฌ ๐——๐—ฎ๐˜†๐˜€ โ€ข ๐Ÿฏ๐Ÿฌ ๐—–๐—ผ๐—ป๐—ฐ๐—ฒ๐—ฝ๐˜๐˜€ ๐—ผ๐—ณ ๐—ค๐˜‚๐—ฎ๐—ป๐˜๐˜‚๐—บ ๐—–๐—ผ๐—บ๐—ฝ๐˜‚๐˜๐—ถ๐—ป๐—ด | ๐——๐—ฎ๐˜† ๐Ÿฎ๐Ÿณ

2 min readAug 9, 2026

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Hello everyone! ๐Ÿ‘‹

Welcome back to Day 27 of the 30 Days โ€ข 30 Concepts of Quantum Computing series.

In the previous blog, we explored Quantum Key Distribution (BB84) and saw how quantum mechanics can secure communication.

Today, weโ€™ll meet the most famous entangled states in quantum computing.

๐—•๐—ฒ๐—น๐—น ๐—ฆ๐˜๐—ฎ๐˜๐—ฒ๐˜€

Bell states are special two-qubit states in which the qubits are perfectly entangled.

They are often called maximally entangled states.

๐—ช๐—ต๐—ฎ๐˜ ๐——๐—ผ๐—ฒ๐˜€ โ€œ๐— ๐—ฎ๐˜…๐—ถ๐—บ๐—ฎ๐—น๐—น๐˜† ๐—˜๐—ป๐˜๐—ฎ๐—ป๐—ด๐—น๐—ฒ๐—ฑโ€ ๐— ๐—ฒ๐—ฎ๐—ป?

Imagine two magical coins.

You toss them far apart.

Whenever you look at them, their results are perfectly related.

If one shows Heads, the other instantly has the matching outcome required by the Bell state.

Neither coin had a fixed value before measurement, yet their results are strongly correlated.

Bell states create this strongest possible quantum correlation.

๐—ง๐—ต๐—ฒ ๐—™๐—ผ๐˜‚๐—ฟ ๐—•๐—ฒ๐—น๐—น ๐—ฆ๐˜๐—ฎ๐˜๐—ฒ๐˜€

Quantum mechanics allows exactly four basic Bell states:

ฮฆ+ = (|00โŸฉ + |11โŸฉ) / โˆš2

ฮฆโˆ’ = (|00โŸฉ โˆ’ |11โŸฉ) / โˆš2

ฮจ+ = (|01โŸฉ + |10โŸฉ) / โˆš2

ฮจโˆ’ = (|01โŸฉ โˆ’ |10โŸฉ) / โˆš2

Donโ€™t worry about memorizing the symbols.

The key idea is:

  • ฮฆ states: both qubits tend to give the same result.
  • ฮจ states: the qubits tend to give opposite results.

๐—ง๐—ต๐—ฒ ๐— ๐—ผ๐˜€๐˜ ๐—™๐—ฎ๐—บ๐—ผ๐˜‚๐˜€ ๐—ข๐—ป๐—ฒ

Consider ฮฆโบ.

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Before measurement, the pair is in a superposition of 00 and 11.

When measured:

  • 50% โ†’ 00
  • 50% โ†’ 11

You never get 01 or 10.

The outcomes are perfectly linked.

๐—›๐—ผ๐˜„ ๐—”๐—ฟ๐—ฒ ๐—•๐—ฒ๐—น๐—น ๐—ฆ๐˜๐—ฎ๐˜๐—ฒ๐˜€ ๐—–๐—ฟ๐—ฒ๐—ฎ๐˜๐—ฒ๐—ฑ?

A common method uses two gates:

  • Apply a Hadamard gate (H) to the first qubit.
  • Apply a CNOT gate using the first qubit as control.

This simple circuit transforms two independent qubits into an entangled Bell pair.

Press enter or click to view image in full size

๐—ช๐—ต๐˜† ๐—”๐—ฟ๐—ฒ ๐—ง๐—ต๐—ฒ๐˜† ๐—œ๐—บ๐—ฝ๐—ผ๐—ฟ๐˜๐—ฎ๐—ป๐˜?

Bell states are building blocks for many quantum technologies:

  • Quantum Teleportation
  • Quantum Key Distribution
  • Superdense Coding
  • Quantum Repeaters
  • Quantum Networks

Whenever two distant qubits need to share strong quantum correlations, Bell states are usually involved.

๐ŸŽ‰ ๐—ง๐—ต๐—ฎ๐˜โ€™๐˜€ ๐—œ๐˜ ๐—ณ๐—ผ๐—ฟ ๐——๐—ฎ๐˜† ๐Ÿฎ๐Ÿณ!

Bell states are the simplest and strongest examples of entanglement.

They show that quantum particles can share correlations that have no classical equivalent, making them one of the most important resources in quantum computing and quantum communication.

๐Ÿ’ญ ๐—ง๐—ต๐—ผ๐˜‚๐—ด๐—ต๐˜ ๐—ผ๐—ณ ๐˜๐—ต๐—ฒ ๐——๐—ฎ๐˜†

โ€œEntanglement is not just connection โ€” itโ€™s a shared quantum reality.โ€

๐Ÿ‘€ ๐—–๐—ผ๐—บ๐—ถ๐—ป๐—ด ๐—จ๐—ฝ ๐—ก๐—ฒ๐˜…๐˜โ€ฆ

๐——๐—ฎ๐˜† ๐Ÿฎ๐Ÿด: ๐—ฆ๐˜‚๐—ฝ๐—ฒ๐—ฟ๐—ฑ๐—ฒ๐—ป๐˜€๐—ฒ ๐—–๐—ผ๐—ฑ๐—ถ๐—ป๐—ด โ€” ๐—ฆ๐—ฒ๐—ป๐—ฑ๐—ถ๐—ป๐—ด ๐—ง๐˜„๐—ผ ๐—•๐—ถ๐˜๐˜€ ๐—จ๐˜€๐—ถ๐—ป๐—ด ๐—ข๐—ป๐—ฒ ๐—ค๐˜‚๐—ฏ๐—ถ๐˜

Weโ€™ll see how a shared Bell state allows one qubit to carry two classical bits of information.

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Lokesh P D
Lokesh P D

Written by Lokesh P D

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