text stringlengths 0 8.13M |
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observables. |
Moreover,theconnectionsestablishedbetweenmodelsofmeasurement-based |
quantumcomputation,permitanaturaltranslationofeachone-dimensionalone- |
way quantum computer into a sequence of state transfers. Therefore, by these |
close connections, the measurement-based quantum computer is unified: a one- |
way quantum computer is nothing but a quantum computer based on state |
transfers, in which a large part of the measurements (those independent on |
the program we want to perform) are grouped in a stage of initialization. Note |
that this initialization can be performed using an Ising transformation, which |
is unitary. The initialization produces the cluster state, on which the rest of |
themeasurements(composedofone-qubitmeasurementsonly)areperformedin |
order to complete the computation. |
Final remark. This paper deals with unifying models of quantum computation |
via measurementsonly, and withminimizing universal families of observables. It |
has been submitted to a conference on April 1st, 2004.The authors have recently |
noticed a report posted on arXiv.org, by P. Aliferis and D. W. Leung [10], deal- |
ing with unifying models of quantum computation via measurements only. The |
relations among both approaches are certainly worth investigating further. |
9 |
References |
1. A.Y.Kitaev,A.H.ShenandM.N.Vyalyi.Classical andQuantum Computation, |
American Mathematical Society, 2002. |
2. D.W. Leung. Two-qubit projective measurements are universal for quantum com- |
putation, arXiv.org report quant-ph/0111077, 2001. |
3. D. W. Leung. Quantum computation by measurements, arXiv.org report |
quant-ph/0310189, 2003. |
4. M. A. Nielsen. Universal quantum computation using only projective mea- |
surement, quantum memory, and preparation of the 0 state, arXiv.org report |
quant-ph/0108020, 2001. |
5. M.A.NielsenandI.L.Chuang.QuantumComputationandQuantumInformation, |
Cambridge University Press, 2000. |
6. S.PerdrixState Transfer instead of Teleportation inMeasurement-based Quantum |
Computation , arXiv.org report quant-ph/0402204, 2004. |
7. R. Raussendorf and H. J. Briegel. Quantum computing via measurements only |
Phys.Rev.Lett. 86 5188, 2000. |
8. R. Raussendorf, D. E. Browne and H. J. Briegel. Measurement-based quantum |
computation with cluster states, arXiv,quant-ph/0301052, 2003. |
9. F.Verstraete,J.I.Cirac.ValenceBondSolidsforQuantumComputation,arXiv.org |
report quant-ph/0311130, 2003. |
10. P. Aliferis, D. W. Leung. Computation by measurements: a unifying picture, |
arXiv.org report quant-ph/0404082, 2004. |
--- End of pdfs/document_6.pdf --- |
--- Start of pdfs/document_7.pdf --- |
Measurement-only verifiable blind quantum computing with quantum input |
verification |
Tomoyuki Morimae1,∗ |
1ASRLD Unit, Gunma University, 1-5-1 Tenjin-cho Kiryu-shi Gunma-ken, 376-0052, Japan |
Verifiableblindquantumcomputingisasecuredelegatedquantumcomputingwhereaclientwith |
a limited quantum technology delegates her quantum computing to a server who has a universal |
quantumcomputer. Theclient’s privacyisprotected (blindness)andthecorrectness ofthecompu- |
tationisverifiablebytheclientinspiteofherlimitedquantumtechnology(verifiability). Thereare |
mainlytwotypesofprotocolsforverifiableblindquantumcomputing: theprotocolwheretheclient |
has only to generate single-qubit states, and the protocol where the client needs only the ability |
6102 of single-qubit measurements. The latter is called the measurement-only verifiable blind quantum |
computing. If the input of the client’s quantum computing is a quantum state whose classical ef- |
ficient description is not known to the client, there was no way for the measurement-only client to |
verifythecorrectnessoftheinput. Hereweintroduceanewprotocolofmeasurement-onlyverifiable |
nuJ blind quantumcomputing where thecorrectness of the quantuminput is also verifiable. |
I. INTRODUCTION ifiability: although the blindness guarantees that Bob |
12 |
cannot learn Alice’s quantum computing, he can still |
deviate from the correct procedure, mess up her quan- |
Blind quantum computing is a secure delegated quan- |
]hp-tnauq[ tum computing, and give Alice a completely wrong re- |
tum computingwhere aclient(Alice) whodoes nothave |
sult. Since Alice cannotperformquantumcomputing by |
enoughquantumtechnologydelegatesherquantumcom- |
herself, she cannot check the correctness of the result by |
puting to a server (Bob) who has a universal quan- |
herself unless the problem is, say, in NP, and therefore |
tum computer without leaking any information about |
shecanacceptawrongresult. Tosolvetheproblem,veri- |
her quantum computing. By using measurement-based |
fiableblindquantumcomputingprotocolwasintroduced |
quantum computing [1, 2], Broadbent, Fitzsimons, and |
inRef.[16],andsometheoreticalimprovementswerealso |
Kashefi first showed that blind quantum computing is |
obtained [17–19]. Experimental demonstrations of the |
indeed possible for a client who can do only the single |
1v76460.6061:viXra qubitstategeneration[3]. Sincethebreakthrough,many verification were also done [20, 21]. The basic idea of |
theseprotocolsissocalledthetraptechnique: Alicehides |
theoreticalimprovementshavebeenobtained[4–12],and |
sometrapqubitsintheregister,andanychangeofatrap |
even a proof-of-principle experiment was achieved with |
signals Bob’s malicious behavior. By checking traps, Al- |
photonic qubits [13]. These blind quantum computing |
ice can detect any Bob’s malicious behavior with high |
protocols guarantee two properties: first, if Bob is hon- |
probability. Ifthecomputationisencodedbyaquantum |
est, Alice can obtain the correct result of her quantum |
error detection code, the probability that Alice is fooled |
computing (correctness). Second, whatever Bob does, |
by Bob can be exponentially small, since in that case in |
he cannot gain any information about Alice’s quantum |
orderto changethe logicalstate, Bobhastotouchmany |
computing (blindness) [14]. |
qubits,anditconsequentlyincreasestheprobabilitythat |
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