text stringlengths 0 8.13M |
|---|
| i | i |
the auxiliary qubit. The (n+1) qubits are guided into |
j the beginning of the circuit, as input state. The process |
will continue until a result is read-out in the conditional |
measurement device. |
0 |
This simulation of duality computer also provides a |
relativity view regarding quantum computer. In a du- |
ality computer, a double-slit is located statically, and a |
quantum computer is moving. However in the duality |
FIG. 3: Schematic illustration of a recycling duality compu- mode,aquantumcomputerisstatic,andthedouble-slit, |
tation. After the auxiliary-qubit-conditioned measurement, |
theauxiliaryqubit,changestosimulatethemotionofthe |
if a result is obtained, the calculation is completed and the |
double-slit. Tomakeaquantumcomputermovingisvery |
process is stopped. If no result is obtained, it destroys the |
difficult, however it is much easier to add one additional |
statein|0i auxiliaryqubit,andleavesastatewheretheaux- |
qubit to an n-qubit quantum computer. |
iliary is in state |1i. The state is restored to the input state |
by a unitary operation V and guided to the input end. The In summary we have given a quantum computer real- |
calculation processisrepeatedagainandagain untilthefinal ization of the duality computer. This realization itself |
result is obtained. servesasanewmodeofquantumcomputing,theduality |
mode. This provides a way to run classical algorithm in |
quantumcomputersusingmuchreducedqubitresources. |
Italsoprovidesamethodforerrorcorrectioninaduality |
After the conditional-measurement, if a result is ob- |
computer. With conditional measurement, the recycling |
tained, the wave-function is collapsed, and the (U0 + |
quantum computing mode is also proposed. These two |
U1)ϕ result is read out. If no-result is obtained, then |
modesprovidenewwaysandflexibilityinquantumalgo- |
| i |
the state in 0 collapses out, and the wave-function be- |
rithm designs. |
| i |
comes |
Acknowledgement |
U0 U1 Helpful discussions with Prof. Dieter Suter and Dr |
ψ ′ =N ′ − ϕ 1 , Qing-Yu Cai are gratefully acknowledged. This work is |
| i 2 | i| i |
supported by the National Fundamental Research Pro- |
where N is a renormalization constant. Then perform- gramGrantNo. 2006CB921106,ChinaNationalNatural |
′ |
ing a unitary operation V on the n qubits, the initial Science Foundation Grant Nos. 10325521,60433050. |
[1] Shor, P W. Algorithms for quantum computation: dis- cessing, 6(1): 49-54, (2007) |
crete logarithms and factoring. In: Proceedings of the [7] Long,GLandLiu,Y,Searchanunsorteddatabasewith |
Symposium on the Foundations of computer Science. quantum mechanics. Front. Comput. Sci. China, 1 (3): |
NewYork: IEEEComputerSocietyPress,1994,124-134. 247-271 (2007) |
[2] Grover, L K, A fast quantum mechanical algorithm for [8] Brassard,G,Hoyer,P,Mosca,MandTapp,A,Quantum |
database search. In: Proceedings of 28th Annual ACM amplitude amplification and esti-mation. AMS Contem- |
Symposium on Theory of Computing. New York: ACM, poraryMathematicsSeriesVol.305,eds.S.J.Lomonaco |
212-219 (1996). and H.E. Brandt, AMS (Providence), p.53, (2002) |
[3] Long, G L, The general quantum interference principle [9] Hoyer,P,Arbitraryphasesinquantumamplitudeampli- |
and the duality computer. Commun. Theor. Phys. 45, fication. Phys.Rev. A 62, 052304 (2001). |
825-844 (2006) . [10] Long,GL,Groveralgorithmwithzerofailurerate,Phys. |
[4] Wang, W Y, Shang, B, Wang, C and Long, G L, Prime Rev. A64, 022307 (2001). |
factorization in the duality computer. Commun. Theor. [11] Grover, L K, Fixed-point quantum search, Phys. Rev. |
Phys.47, 471-473 (2007). Lett. 95, 150501 (2005). |
[5] Gudder,S,Dualityquantumcomputers.QuantumInfor- [12] Shor,PW,Schemeforreducingdecoherenceinquantum |
mation Processing, 6 (1): 49-54, (2007). computer memory. Phys.Rev.A. 52, R2493 (1995). |
[6] Long, G L, Mathematical theory of duality computer in |
thedensitymatrixformalism.QuantumInformationPro- |
--- End of pdfs/document_10.pdf --- |
--- Start of pdfs/document_11.pdf --- |
CLASSICAL COMPUTING, QUANTUM COMPUTING, |
AND SHOR’S FACTORING ALGORITHM1 |
Yu. I. Manin |
Max–Planck–Institut fu¨r Mathematik, Bonn, Germany |
0. Why quantum computing? |
9991 |
Information processing (computing) is the dynamical evolution of a highly orga- |
nized physical system produced by technology (computer) or nature (brain). The |
raM |
initial state of this system is (determined by) its input; its final state is the output. |
Physics describes nature in two complementary modes: classical and quantum. Up |
to the nineties, the basic mathematical models of computing, Turing machines, |
2 |
were classical objects, although the first suggestions for studying quantum models |
1v8003099/hp-tnauq:viXra date back at least to 1980. |
Roughly speaking, the motivation to study quantum computing comes from |
several sources: physics and technology, cognitive science, and mathematics. We |
will briefly discuss them in turn. |
(i) Physically, the quantum mode of description is more fundamental than the |
classical one. In the seventies and eighties it was remarked that, because of the |
superposition principle, it is computationally unfeasible to simulate quantum pro- |
cesses on classical computers ([Po], [Fe1]). Roughly speaking, quantizing a classical |
system with N states we obtain a quantum system whose state space is an (N 1)– |
− |
dimensional complex projective space whose volume grows exponentially with N. |
One can argue that the main preoccupation of quantum chemistry is the struggle |
with resulting difficulties. Reversing this argument, one might expect that quan- |
tum computers, if they can be built at all, will be considerably more powerful than |
classical ones ([Fe1], [Ma2]). |
Progress in the microfabrication techniques of modern computers has already led |
us to the level where quantum noise becomes an essential hindrance to the error– |
free functioning of microchips. It is only logical to start exploiting the essential |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.