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Qudits of Multi-Single Slits, Multi-Double Slits and Multi-Triple Slits

Hui Peng, James Peng

Published Feb 21, 2024• 0 citations
Publisher

Abstract

One of tasks of quantum computing research is to reduce the components. We propose four kinds of Qudits, respectively formed by: (1) multi-single-slits; (2) multi-double-slits (multi-Qubits); (3) multi-triple-slits (multi-Qutrits); and (4) combination of (1), (2), (3).
DOI
10.1364/opticaopen.25230485.v2

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•Jun 13, 2011•0 citations
One of tasks of quantum computing research is to reduce the components utilized for reaching certain computation power. To significantly reduce the components, we propose four kinds of Qudits of higher-dimension, multi-folds higher than the two-dimension of the qubits, which are respectively formed by: (1) multi-single-slits; (2) multi-double-slits (multi-Qubits); (3) multi-triple-slits (multi-Qutrits); and (4) combination of above. The further advantage is that the so formed Qudits may adopt Octal Number System, Decimal Number System, Duodecimal Number System, and Hexadecimal Number System, respectively.
Abstract Quantum computing leverages the power of superposition, entanglement, and interference to surpass classical systems in certain computational tasks. The first studies revolved around two-state quantum systems (qubits), which are a superposition of the |0⟩ and |1⟩ states. These qubits are physically realized using subatomic particles (e.g., electrons or photons) with the two states corresponding to different energy levels or polarization directions. However, some of these particles can exist in more than two discrete states. For example, an electron may occupy several energy levels, or a photon may have more than two polarization states. As a result, there has been an interest in qudits, quantum systems with d different states. A fascinating subcase of this is a qutrit, a three-level quantum system with states |0⟩, |1⟩, and |2⟩ as its basis. It is understood that qutrits with their larger state space can improve the storage and processing of information, and Qutrit-based quantum computing can be realized by defining suitable quantum gates to concatenate the three-level systems. Researchers have proposed qutrit gates, some of which are direct generalizations of qubit gates, such as the Pauli-X gate, and others are entirely new gate constructs. This paper summarizes recent advances in qutrit-based quantum computing, where the definitions of various qutrit gates are presented, and their significance in the development of qutrit-based quantum computing, particularly in implementing Deutsch and Shor’s algorithms, is explored.
Qudit is a multi-level computational unit alternative to the conventional 2-level qubit. Compared to qubit, qudit provides a larger state space to store and process information, and thus can provide reduction of the circuit complexity, simplification of the experimental setup and enhancement of the algorithm efficiency. This review provides an overview of qudit-based quantum computing covering a variety of topics ranging from circuit building, algorithm design, to experimental methods. We first discuss the qudit gate universality and a variety of qudit gates including the pi/8 gate, the SWAP gate, and the multi-level-controlled gate. We then present the qudit version of several representative quantum algorithms including the Deutsch-Jozsa algorithm, the quantum Fourier transform, and the phase estimation algorithm. Finally we discuss various physical realizations for qudit computation such as the photonic platform, iron trap, and nuclear magnetic resonance.
During the past thirty years the field of Quantum Information has beenvery successful in proposing protocols and algorithms that involve two-level quantum systems known as qubits. It has been shown that cryptographic keys can be distributed securely using quantum resources and that quantum algorithms can solve tasks such as the factoring of large numbers with an exponential speedup over classical algorithms. Most implementations, however, are restricted to proof-of-concept experiments using few qubits, due to the difficulty of scaling the physical systems utilized. Quantum systems with more than two levels, called qudits, present themselves as an alternative way of obtaining a space with large dimensionality without recurring to a large number of qubits. This reduces the number of particles necessary for implementing protocols in a scale that is relevant for practical applications. Additionally, pairs of entangled qudits are more robust agains noise than their qubit counterparts and are also more adequate for experiments that test the non-local and contextual behavior of nature, as predicted by its description using Quantum Mechanics. In this thesis we present the construction and characterization of a source of states of four qudits. We used a pulsed laser as pump for type-II Spontaneous Parametric Down Conversion (SPDC) to occur on a PPKTP, a KTiOPO4 (KTP) crystal with a periodic ferroelectric domain inversion, a technique called periodic poling. In type-II SPDC a pair of photons, also called biphoton, is generated in which one has horizontal polarization while the other hasvertical polarization. Due to the use of a pulsed pump beam and the highdown-conversion efficiency of our PPKTP, the probability that a single pump pulse will originate two pairs of photons is high. In order to generate qudits we used the multiple-slit implementation, meaning that a multiple slit was placed between the PPKTP and the detectors, encoding discrete qudit states onto the continuous transverse mode of the biphoton. Using double, triple and quadruple slits we produced, respectively, qubit, qutrit and ququart states. A system of lenses placed between the PPKTP and the slits manipulated the amplitude of the transverse biphoton state impinging on the slits and, thus, the quantum correlations between qudits after the slits. By projecting either the near or far field of the crystal onto the slits, the lenses changed the characteristics of the biphoton amplitude function and allowed us to obtain either states with very high entanglement, in the case of the near field, or very low entanglement, in the case of the far field. A lens in the f-f configuration between the plane of the slits and the plane of the detectors projected the far field of the slits, so we could observe conditional interference patterns. We detected the photons in coincidence asa function of the position of two detectors These were used to generate maps of coincidences between two photons with different polarization and for two photons with the same polarization. The first case contains contributions from photons of a single pair and from photons from two different pairs, while the second case contains contributions from different pairs only. In order to isolate the single pair contribution on different-polarization coincidences, we removed the background component from photons of different pairs, given by the same-polarization coincidences. Besides serving to isolate the singlepair signal, same-polarization coincidences confirm the existence two-pair events and give us information about the purity of the reduced state of a single photon, which is related to the degree of entanglement in a biphoton. We conclude that manipulating the biphoton transverse amplitude is a promising technique for generating qudit states while controlling their entanglement and correlation properties, especially if more exotic transverse amplitudes are explored, such as Hermite-Gaussian pump beams or amplitudes engineered with a spatial light modulator. The use of high-efficiency SPDC sources allows for states of more than one biphoton, engineered using transverse amplitude manipulation, to be employed in many different protocolsin Quantum Information, serving as sources of heralded pure or mixedstates, or playing an important role in tests of the non-local and contextual nature of physical systems, as predicted by Quantum Mechanics.