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Lokesh P D

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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Ÿด

3 min readAug 9, 2026

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Hello everyone!

Welcome back to Day 28 of the 30 Days โ€ข 30 Concepts of Quantum Computing series.

In the previous blog, we explored Bell States and learned how two qubits can become perfectly entangled.

Today, weโ€™ll see a surprising application of entanglement.

๐—ฆ๐˜‚๐—ฝ๐—ฒ๐—ฟ๐—ฑ๐—ฒ๐—ป๐˜€๐—ฒ ๐—–๐—ผ๐—ฑ๐—ถ๐—ป๐—ด

What if I told you that one qubit can carry two classical bits of information?

That sounds impossible because a classical bit can store only 0 or 1.

But with a shared Bell state, quantum mechanics allows something remarkable.

๐—ง๐—ต๐—ฒ ๐—•๐—ฎ๐˜€๐—ถ๐—ฐ ๐—œ๐—ฑ๐—ฒ๐—ฎ

Alice and Bob first share an entangled Bell pair.

Alice keeps one qubit.

Bob keeps the other.

To send a message, Alice performs a quantum operation on her qubit only and then sends that single qubit to Bob.

Bob performs a joint measurement on both qubits and can determine which operation Alice used.

That operation corresponds to two classical bits.

๐—›๐—ผ๐˜„ ๐—ง๐˜„๐—ผ ๐—•๐—ถ๐˜๐˜€ ๐—”๐—ฟ๐—ฒ ๐—˜๐—ป๐—ฐ๐—ผ๐—ฑ๐—ฒ๐—ฑ

Using one shared Bell state, Alice can choose among four operations:

  • I โ†’ 00
  • X โ†’ 01
  • Z โ†’ 10
  • XZ โ†’ 11

Each operation transforms the Bell state into a different Bell state.

After receiving Aliceโ€™s qubit, Bob measures the pair and learns which of the four states he has.

From that, he recovers the two-bit message.

๐—” ๐—ฅ๐—ฒ๐—ฎ๐—น-๐—Ÿ๐—ถ๐—ณ๐—ฒ ๐—”๐—ป๐—ฎ๐—น๐—ผ๐—ด๐˜†

Imagine Alice and Bob each hold half of a special lock.

The lock was prepared together beforehand.

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By making one of four small adjustments to her half and sending it to Bob, the complete lock reveals one of four distinct patterns.

Four possible patterns can represent 00, 01, 10, or 11.

The extra information comes from the shared entanglement, not from the traveling qubit alone.

๐—ช๐—ต๐˜† ๐—œ๐˜€ ๐—ง๐—ต๐—ถ๐˜€ ๐—ฆ๐˜‚๐—ฟ๐—ฝ๐—ฟ๐—ถ๐˜€๐—ถ๐—ป๐—ด?

A qubit by itself cannot reveal two classical bits when measured.

The trick is that Alice and Bob already share entanglement before communication begins.

Entanglement acts like a pre-shared quantum resource, allowing one transmitted qubit to unlock two bits of classical information.

๐—ช๐—ต๐˜† ๐—œ๐˜€ ๐—œ๐˜ ๐—œ๐—บ๐—ฝ๐—ผ๐—ฟ๐˜๐—ฎ๐—ป๐˜?

Superdense Coding is important for:

  • Quantum communication
  • Quantum networks
  • Entanglement-based communication protocols
  • Efficient information transfer

It demonstrates that entanglement can increase communication efficiency, something impossible in classical physics.

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๐——๐—ผ๐—ฒ๐˜€ ๐—œ๐˜ ๐—ฉ๐—ถ๐—ผ๐—น๐—ฎ๐˜๐—ฒ ๐—ฃ๐—ต๐˜†๐˜€๐—ถ๐—ฐ๐˜€?

No.

Alice still sends one physical qubit to Bob.

The additional information capacity comes from the entangled pair they prepared earlier.

No information travels faster than light.

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

Superdense Coding shows that entanglement is not just a curious quantum effect โ€” it can become a practical communication resource.

By combining a shared Bell state with a single transmitted qubit, two classical bits can be communicated efficiently.

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

โ€œEntanglement turns a single qubit into a richer communication channel.โ€

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

๐——๐—ฎ๐˜† ๐Ÿฎ๐Ÿต: ๐—ค๐˜‚๐—ฎ๐—ป๐˜๐˜‚๐—บ ๐—ฆ๐˜‚๐—ฝ๐—ฟ๐—ฒ๐—บ๐—ฎ๐—ฐ๐˜† ๐˜ƒ๐˜€ ๐—ค๐˜‚๐—ฎ๐—ป๐˜๐˜‚๐—บ ๐—”๐—ฑ๐˜ƒ๐—ฎ๐—ป๐˜๐—ฎ๐—ด๐—ฒ

Weโ€™ll learn the difference between performing a task that is practically impossible for classical computers and performing a task that is simply better on a quantum computer.

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Lokesh P D
Lokesh P D

Written by Lokesh P D

Stay Hungry, Stay Curious