Answers:
量子门隐形传态是在隐形状态下能够将量子门应用于未知状态的行为。这是可以使用图形状态描述基于度量的计算的方式之一。
通常,隐形传态通过具有未知的量子态而起作用爱丽丝举行,并在贝尔状态两个量子比特爱丽丝(Alice)和鲍勃(Bob)之间共享 2个。爱丽丝进行贝尔状态测量,获取4个可能答案之一,而鲍勃则根据其4个状态之一的爱丽丝的测量结果保持其量子位因此,一旦鲍勃了解爱丽丝得到了什么结果,他就可以通过应用适当的宝利斯来进行补偿。
令为1量子位unit。假设Alice和Bob份额代替。如果他们重复传送协议,则Bob现在将具有之一。ψ ⟩ ,û X | ψ ⟩ ,ü ž | ψ ⟩ ,ü ž X | ψ ⟩,我们可以改写为
即使您不仅需要Pauli门(的情况也是如此)), the compensations may be easier than implementing the gate directly. This is the basis of the construction of the fault-tolerant T gate.
In fact, you can do something similar to apply a controlled-NOT between a pair of qubits as well. This time, the state you need is , and a controlled-NOT applied between and . This time, there are 16 possible compensating rotations, but all of them are just about how Pauli operations propagate through the action of a controlled-NOT and, again, that just gives Pauli operations out.
Gate teleportation is in principle a method that allows the creation of different gates from an available set of gates, by teleporting qubits through entangled states. An example of the use of this method, is the creation of the T gate from a Clifford set of gates in order to make the set universal. The construction in this particular case is done with the use of special T ancillae. The standard reference can be found in arXiv:quant-ph/9908010.
For simulating quantum circuits you can use the gate teleportation to move gates around the circuit with the use of ancillae qubit (number of ancillae depended on the number of gates).