Difference between revisions of "JQ Manual"

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=== 1st text input - init state ===
 
=== 1st text input - init state ===
 
[[File:1st.png]]
 
[[File:1st.png]]
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You enter init state of qubits here. Decimal integer is required here. Its binary representation defines start states of qubits. **Qubit 0 is on the top**.
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=== 2nd text input - qubit signature ===
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[[File:2nd.png]]
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You enter list of integers here in the following format: [qubit1, qubit2, ..., qubitn]. This bit signature is used for displaying probabilities.
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Assume you entered there [3,4] and assume that result probability is like the following:
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<code>
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01 : 0.3 (1)
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10 : 0.7 (2)
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</code>
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It simply means that hypothetical measurement would show that P(qubit 4 is in state 0 AND qubit 3 is in state 1) = 0.3 and P(qubit 4 is in state 1 AND qubit 3 is in state 0) = 0.7.
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So the results is simply a list of numbers with certain probability. The n-th bit of number (from right) represents state of n-th quibit in signature (from left) after hypothetical measurment.

Revision as of 12:31, 20 May 2013

Quick Overview

For quick start, please note 3 text input. We we will name the 1st, 2nd and 3rd -- from left to right. Please also note 2 buttons: Run and Load.

1st text input - init state

1st.png You enter init state of qubits here. Decimal integer is required here. Its binary representation defines start states of qubits. **Qubit 0 is on the top**.

2nd text input - qubit signature

2nd.png You enter list of integers here in the following format: [qubit1, qubit2, ..., qubitn]. This bit signature is used for displaying probabilities.

Assume you entered there [3,4] and assume that result probability is like the following: 01 : 0.3 (1) 10 : 0.7 (2)

It simply means that hypothetical measurement would show that P(qubit 4 is in state 0 AND qubit 3 is in state 1) = 0.3 and P(qubit 4 is in state 1 AND qubit 3 is in state 0) = 0.7. So the results is simply a list of numbers with certain probability. The n-th bit of number (from right) represents state of n-th quibit in signature (from left) after hypothetical measurment.

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