| Contents | Summary | Panvia Quantum Computer | Quail | Method | ||||
|---|---|---|---|---|---|---|---|---|
| Alice | Eve | Bob | ||||||
| Results | Applications |
Alice's circuits starting states Bob's circuits ending states | english latin korean > | hmong swahili german > Alice's 1st qubit state english number has been teleported via a randomized state superposition to Bob's 3rd qubit state german number. zero 100% |0> null 100% |0> one 85% |0> + 15% |1> eins 85% |0> + 15% |1> two 50% |0> + 50% |1> zwei 50% |0> + 50% |1> three 15% |0> + 85% |1> drei 15% |0> + 85% |1> four 100% |1> vier 100% |1> the zero ... four pattern is repeated in the interval five ... nine This shows that Alice's second qubit latin state |1> versus |0> has no effect on the teleportation process. For Alice's circuits ten to nineteen the 3rd qubit in korean is |1> The result observed is a reflection in |0> |1> sense of the quantum state teleported to Bob's german qubit so the pattern of light versus dark in the ten to nineteen interval is a reflection of of the pattern from zero to nine. ten 100% |1> zehn 100% |1> eleven 85% |1> + 15% |0> elf 85% |1> + 15% |0> twelve 50% |1> + 50% |0> zwolf 50% |1> + 50% |0> thirteen 15% |1> + 85% |0> dreizehn 15% |1> + 85% |0> fourteen 100% |0> vierzehn 100% |0>
A third party 'Eve' cannot eavesdrop between Alice's circuit and Bob's circuit since in each of the 41 circuits all 3 qubits have been scrambled into superpositions of 50% of |0> and 50% of |1>Alice's circuits ending states = Bob's circuits starting states | english latin korean > | hmong swahili german > Alice's 1st qubit state english number is a state superposition of |0> and |1> as is Bob's 3rd qubit state german number. zero 50% |0> + 50% |1> = |000> 25% + |011> 25% + |100> 25% + |111> 25% = null 50% |0> + 50% |1>
| | zero, nihil, yeong > | | x x x > | probability |
| blue | | 0 0 0 > | 25% |
| sand | | 0 1 1 > | 25% |
| green | | 1 0 0 > | 25% |
| pink | | 1 1 1 > | 25% |
| | | x | x | x | > | probability | ||
| blue | | | 0 | 0 | 0 | > | 25% | |
| sand | | | 0 | 1 | 1 | > | 25% | |
| green | | | 1 | 0 | 0 | > | 25% | |
| pink | | | 1 | 1 | 1 | > | 25% | |
| total |0> | 50% |0> | 50% |0> | 50% |0> | 50% | |||
| total |1> | 50% |1> | 50% |1> | 50% |1> | 50% |
The probability of each qubit is 50% |0> and 50% |1>. Any measurement of any qubit will have a 50% probability of either state being observed so will generate a random 0 or 1. In the process of measuring any selected qubit the other two qubits, each of which is in a 50%:50% superposition of |0> and |1> states, will also randomly collapse to either 0 or 1 with equal likelihood. This because the collapsed state has to be 100% of one of the four quantum state superposition possibilities |000>, |011>, |100> or |111>.
| | xoom, sufuri, null > | | x x x > | probability |
| blue | | 0 0 0 > | 25% |
| sand | | 0 1 1 > | 25% |
| green | | 1 0 0 > | 25% |
| pink | | 1 1 1 > | 25% |