2000
DOI: 10.1145/367701.367709
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An introduction to quantum computing for non-physicists

Abstract: Richard Feynman's observation that certain quantum mechanical effects cannot be simulated efficiently on a computer led to speculation that computation in general could be done more efficiently if it used these quantum effects. This speculation proved justified when Peter Shor described a polynomial time quantum algorithm for factoring integers.In quantum systems, the computational space increases exponentially with the size of the system which enables exponential parallelism. This parallelism could lead to ex… Show more

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Cited by 262 publications
(208 citation statements)
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“…Then the GHZ-like can be generated successfully. In fact, C-NOT gate operation [20], the generations of single photon and Bell state [21] have already been well demonstrated experimentally. Thus, the preparation of GHZ-like state is also feasible and it can be well demonstrated experimentally within the present technology.…”
Section: Preparation Of Ghz-like Statementioning
confidence: 97%
“…Then the GHZ-like can be generated successfully. In fact, C-NOT gate operation [20], the generations of single photon and Bell state [21] have already been well demonstrated experimentally. Thus, the preparation of GHZ-like state is also feasible and it can be well demonstrated experimentally within the present technology.…”
Section: Preparation Of Ghz-like Statementioning
confidence: 97%
“…More detailed presentations can be found in the books by Gruska (1999) and Nielsen & Chuang (2000). Rieffel and Polak (2000) give an account aimed at computer scientists, and Preskill's (1998) lecture notes are another valuable resource. Arrighi (2003) covers similar material to this section, with a more detailed discussion of the fundamentals of quantum theory.…”
Section: Basics Of Quantum Computingmentioning
confidence: 99%
“…Below is a simplified example [12,18] of the quantum error correction using encoding. The simplification results from the assumption that the only errors allowed are rotations around the x axis, described by the matrix E = cos(θ/2)I − i sin(θ/2)σ x , where I is the unit matrix and σ x is the Pauli matrix.…”
Section: Quantum Error Correction By Encodingmentioning
confidence: 99%