๐ ๐ฏ๐ฌ ๐๐ฎ๐๐ โข ๐ฏ๐ฌ ๐๐ผ๐ป๐ฐ๐ฒ๐ฝ๐๐ ๐ผ๐ณ ๐ค๐๐ฎ๐ป๐๐๐บ ๐๐ผ๐บ๐ฝ๐๐๐ถ๐ป๐ด | ๐๐ฎ๐ ๐ฎ๐ณ
Hello everyone! ๐
Welcome back to Day 27 of the 30 Days โข 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, weโll meet the most famous entangled states in quantum computing.
๐๐ฒ๐น๐น ๐ฆ๐๐ฎ๐๐ฒ๐
Bell states are special two-qubit states in which the qubits are perfectly entangled.
They are often called maximally entangled states.
๐ช๐ต๐ฎ๐ ๐๐ผ๐ฒ๐ โ๐ ๐ฎ๐ ๐ถ๐บ๐ฎ๐น๐น๐ ๐๐ป๐๐ฎ๐ป๐ด๐น๐ฒ๐ฑโ ๐ ๐ฒ๐ฎ๐ป?
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.
๐ง๐ต๐ฒ ๐๐ผ๐๐ฟ ๐๐ฒ๐น๐น ๐ฆ๐๐ฎ๐๐ฒ๐
Quantum mechanics allows exactly four basic Bell states:
ฮฆ+ = (|00โฉ + |11โฉ) / โ2
ฮฆโ = (|00โฉ โ |11โฉ) / โ2
ฮจ+ = (|01โฉ + |10โฉ) / โ2
ฮจโ = (|01โฉ โ |10โฉ) / โ2
Donโt 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.
๐ง๐ต๐ฒ ๐ ๐ผ๐๐ ๐๐ฎ๐บ๐ผ๐๐ ๐ข๐ป๐ฒ
Consider ฮฆโบ.
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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.
๐๐ผ๐ ๐๐ฟ๐ฒ ๐๐ฒ๐น๐น ๐ฆ๐๐ฎ๐๐ฒ๐ ๐๐ฟ๐ฒ๐ฎ๐๐ฒ๐ฑ?
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.
๐ช๐ต๐ ๐๐ฟ๐ฒ ๐ง๐ต๐ฒ๐ ๐๐บ๐ฝ๐ผ๐ฟ๐๐ฎ๐ป๐?
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.
๐ ๐ง๐ต๐ฎ๐โ๐ ๐๐ ๐ณ๐ผ๐ฟ ๐๐ฎ๐ ๐ฎ๐ณ!
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.
๐ญ ๐ง๐ต๐ผ๐๐ด๐ต๐ ๐ผ๐ณ ๐๐ต๐ฒ ๐๐ฎ๐
โEntanglement is not just connection โ itโs a shared quantum reality.โ
๐ ๐๐ผ๐บ๐ถ๐ป๐ด ๐จ๐ฝ ๐ก๐ฒ๐ ๐โฆ
๐๐ฎ๐ ๐ฎ๐ด: ๐ฆ๐๐ฝ๐ฒ๐ฟ๐ฑ๐ฒ๐ป๐๐ฒ ๐๐ผ๐ฑ๐ถ๐ป๐ด โ ๐ฆ๐ฒ๐ป๐ฑ๐ถ๐ป๐ด ๐ง๐๐ผ ๐๐ถ๐๐ ๐จ๐๐ถ๐ป๐ด ๐ข๐ป๐ฒ ๐ค๐๐ฏ๐ถ๐
Weโll see how a shared Bell state allows one qubit to carry two classical bits of information.








