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If C(1)=P, C(2)=C, C(3)=T, then
If C(1)=P, C(2)=C, C(3)=T, then
C(n)={U:UQU\dagger=C(n-1),Q\epsilon C(1)}
C(n)={U:UQU\dagger=C(n-1),Q\epsilon C(1)}
 
==Classical Quantum State
== Homomorphic Encryption ==
==Density Matrices==
 
== Quantum One Time Pad ==
== Quantum One Time Pad ==
 
===Pauli Gates===
===Clifford Gates===
===T Gates===
==Discrete Variables and Continuous Variables==


== Measurement Based Quantum Computation (MBQC)==
== Measurement Based Quantum Computation (MBQC)==
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X4s3Z4s2Z1s2M3xM2xE13E234{equation missing} <br/>
X4s3Z4s2Z1s2M3xM2xE13E234{equation missing} <br/>
Hence, we obtain a measurement pattern to implement C-NOT gate with a T-shaped graph state with three qubits entangled chain {2,3,4} and 1 entangled to 3. X dependency sets for qubit 1:{s3}, 2:φ, 3:φ, 4:φ. Z dependency sets for qubit 1:{s2}, 2:φ, 3:φ, 4:{s2}. The measurements are independent of any outcome so they can all be performed in parallel. In the end, Pauli corrections are performed as such. Parity (modulo 2 sum) of all the previous outcomes in the dependency set is calculated for each qubit{equation missing} (i), for X (sXi = s1 ⊕ s2 ⊕ ...) and Z (sZi = s1 ⊕ s2 ⊕ ...), separately. Thus,  is operated on qubit i.{equation missing} <br/>
Hence, we obtain a measurement pattern to implement C-NOT gate with a T-shaped graph state with three qubits entangled chain {2,3,4} and 1 entangled to 3. X dependency sets for qubit 1:{s3}, 2:φ, 3:φ, 4:φ. Z dependency sets for qubit 1:{s2}, 2:φ, 3:φ, 4:{s2}. The measurements are independent of any outcome so they can all be performed in parallel. In the end, Pauli corrections are performed as such. Parity (modulo 2 sum) of all the previous outcomes in the dependency set is calculated for each qubit{equation missing} (i), for X (sXi = s1 ⊕ s2 ⊕ ...) and Z (sZi = s1 ⊕ s2 ⊕ ...), separately. Thus,  is operated on qubit i.{equation missing} <br/>
==Classical Methods==
===Learning with errors===
===Trapdoor Claw-free function pair For Quantum Verification===
===Homomorphic Encryption===
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