Quantum memory

In quantum computing, quantum memory is the quantum-mechanical version of ordinary computer memory. Whereas ordinary memory stores information as binary states (represented by "1"s and "0"s), quantum memory stores a quantum state for later retrieval. These states hold useful computational information known as qubits. Unlike the classical memory of everyday computers, the states stored in quantum memory can be in a quantum superposition, giving much more practical flexibility in quantum algorithms than classical information storage.

Quantum memory is essential for the development of many devices in quantum information processing, including a synchronization tool that can match the various processes in a quantum computer, a quantum gate that maintains the identity of any state, and a mechanism for converting predetermined photons into on-demand photons. Quantum memory can be used in many aspects, such as quantum computing and quantum communication. Continuous research and experiments have enabled quantum memory to realize the storage of qubits.[1]

Background and history

The interaction of quantum radiation with multiple particles has sparked scientific interest over the past decade. Quantum memory is one such field, mapping the quantum state of light onto a group of atoms and then restoring it to its original shape. Quantum memory is a key element in information processing, such as optical quantum computing and quantum communication, while opening a new way for the foundation of light-atom interaction. As we all know, restoring the quantum state of light is no easy task. While impressive progress has been made, researchers are still working to make it happen.[2]

Quantum memory based on the quantum exchange is possible to store photon qubits Kessel and Moiseev[3] has discussed quantum storage in the single photon state in 1993. The experiment was analyzed in 1998 and demonstrated in 2003. Basically, the study of quantum storage in the single photon state can be regarded as the product of the classical optical data storage technology proposed in 1979 and 1982. Not only that, but the idea was inspired by the high density of data storage in the mid-1970s. Optical data storage can be achieved by using absorbers to absorb different frequencies of light, which are then directed to beam space points and stored.

Types

Light Quantum Memory

Normal, classical optical signals are transmitted by varying the amplitude of light. In this case, a piece of paper, or a computer hard disk, can be used to store information on the lamp. In the quantum information scenario, however, the information may be encoded according to the amplitude and phase of the light. For some signals, you cannot measure both the amplitude and phase of the light without interfering with the signal. To store quantum information, you need to store the light itself without measuring it. If you measure it, the information is lost. Light for quantum memory is recording the state of light into the atomic cloud. When light is absorbed by atoms, they can input all the information about the quantum of light.[4]

Solid Quantum Memory

In classical computing, memory is a trivial resource that can be replicated in long-lived memory hardware and retrieved later for further processing. In quantum computing, this is forbidden because, according to the clone-free theorem, any quantum state cannot be reproduced completely. Therefore, in the absence of quantum error correction, the storage of qubits is limited by the internal coherence time of the physical qubits holding the information. "Quantum memory" beyond the given physical qubit storage limits, it will be a quantum information transmission to the "storing qubits", "storing qubits" is not easily affected by environmental noise and other factors, and then when needed information back to the preferred "process qubits", to allow rapid operation or read.[5]

Discovery

Optical quantum memory is usually used to detect and store single photon quantum states. However, producing such an efficient memory is still a huge challenge for current science. A single photon is too low in energy to be lost in a complex light background. These problems have long suppressed quantum storage rates below 50%. A team led by professor Du Shengwang of the department of physics at the Hong Kong University of science and technology[6] and William Mong Institute of Nano Science and Technology at HKUST [7] has found a way to increase the efficiency of optical quantum memory to more than 85 percent. The discovery also brings the popularity of quantum computers closer to reality. At the same time, the quantum memory can also be used as a repeater in the quantum network, which lays the foundation for the quantum Internet.

Research and application

Quantum memory is an important component of quantum information processing applications such as quantum network, quantum repeater, linear optical quantum computation or long-distance quantum communication.[8]

Optical data storage has been an important research topic for many years. Its most interesting function is the use of the laws of quantum physics to protect data from theft, through quantum computing and quantum cryptography unconditionally guaranteed communication security.[9]

They allow particles to be superimposed and in a superposition state, which means they can represent multiple combinations at the same time. These particles are called quantum bits, or qubits. From a cybersecurity perspective, the magic of qubits is that if a hacker tries to observe them in transit, their fragile quantum states shatter. This means it is impossible for hackers to tamper with network data without leaving a trace. Now, many companies are taking advantage of this feature to create networks that transmit highly sensitive data. In theory, these networks are secure.[10]

Microwave storage and light learning microwave conversion

The nitrogen-vacancy center in diamond has attracted a lot of research in the past decade due to its excellent performance in optical nanophotonic devices. In a recent experiment, electromagnetically induced transparency was implemented on a multi-pass diamond chip to achieve full photoelectric magnetic field sensing. Despite these closely related experiments, optical storage has yet to be implemented in practice. The existing nitrogen-vacancy center (negative charge and neutral nitrogen-vacancy center) energy level structure makes the optical storage of the diamond nitrogen-vacancy center possible.

The coupling between the nitrogen-vacancy spin ensemble and superconducting qubits provides the possibility for microwave storage of superconducting qubits. Optical storage combines the coupling of electron spin state and superconducting quantum bits, which enables the nitrogen-vacancy center in diamond to play a role in the hybrid quantum system of the mutual conversion of coherent light and microwave.[11]

Orbital angular momentum is stored in basic steam

Large resonant light depth is the premise of constructing efficient quantum-optical memory. Alkali metal vapor isotopes of a large number of near-infrared wavelength optical depth, because they are relatively narrow spectrum line and the number of high density in the warm temperature of 50-100 ∘ C.Alkali vapors have been used in some of the most important memory developments, from early research to the latest results we are discussing, due to their high optical depth, long coherent time and easy near-infrared optical transition.

Because of its high information transmission ability, people are more and more interested in its application in the field of quantum information. Structured light carries the orbital angular momentum, which must be stored in the memory is to faithfully reproduce the stored structural photons. Atomic vapor quantum memory is ideal for storing such beams because the orbital angular momentum of photons can be mapped to the phase and amplitude of the distributed integration excitation. Diffusion is a major limitation of this technique because the motion of hot atoms destroys the spatial coherence of the storage excitation. Early successes included storing weakly coherent pulses of spatial structure in a warm, ultracold atomic whole. In one experiment, the same group of scientists in a two-orbital caesium magneto-optical trap was able to store and retrieve vector beams at the single-photon level, characterized by changes in the plane polarization of the transverse beam. The memory preserves the rotation invariance of the vector beam, making it possible to use it in conjunction with qubits encoded for maladjusted immune quantum communication.

The first storage structure, a real single photon, was achieved with electromagnetically induced transparency in rubidium magneto-optical trap. The predicted single photon generated by spontaneous four-wave mixing in one magneto-optical trap is prepared by an orbital angular momentum unit using spiral phase plates, stored in the second magneto-optical trap and recovered. The dual-orbit setup also proves coherence in multimode memory, where a preannounced single photon stores the orbital angular momentum superposition state for 100 nanoseconds.[12]

Optical Quantum

GEM

GEM(Gradient Echo Memory) is a photonic echo optical storage technology. The idea was first demonstrated by researchers at ANU. Their experiment is a three-level system based on steam. This system is the most efficient we've ever seen in hot steam, up to 87%.[13]

Electromagnetically induced transparency

Electromagnetically induced transparency was first introduced by Harris and his colleagues at Stanford University in 1990.[14] The work shows that when a laser beam causes quantum interference between excitation paths, the optical response of the atomic medium is modified to eliminate absorption and refraction at the resonant frequencies of atomic transitions. Slow light, optical storage, and quantum memory are realized based on electromagnetically induced transparency. Compared to other approaches, the electromagnetically induced transparency approach has a long storage time and is a relatively easy and inexpensive solution to implement. The electromagnetically induced transparency does not require the very high power control beams required for Raman quantum memory, nor does it require specific liquid helium temperatures. In addition, unlike the method based on photon echo, photon echo can read electromagnetically induced transparency while the spin coherence survives due to the time delay of readout pulse caused by a spin recovery in non-uniformly broadened media. Although there are some limitations on operating wavelength, bandwidth, and mode capacity, techniques have been developed to make electromagnetically induced transparency quantum memory feasible in quantum information systems.[15] In 2018, a highly efficient EIT-based quantum memory in cold atom has been demonstrated of 92% storage efficiency, which is the highest record to date.[16]

Crystals doped with rare earth

The mutual transformation of quantum information between light and matter is the focus of quantum informatics. The interaction between a single photon and a cooled crystal doped with rare earth ions is investigated. Crystals doped with rare earth have broad application prospects in the field of quantum storage because they provide a unique application system.[17] Li Chengfeng from the quantum information laboratory of the Chinese Academy of Sciences developed a solid-state quantum memory and demonstrated the photon computing function using time and frequency. Based on this research, a large-scale quantum network based on quantum repeater can be constructed by utilizing the storage and coherence of quantum states in the material system. Researchers have shown for the first time in rare-earth ion-doped crystals. By combining the three-dimensional space with two-dimensional time and two-dimensional spectrum, a kind of memory that is different from the general one is created. It has the multimode capacity and can also be used as a high fidelity quantum converter. Experimental results show that in all these operations, the fidelity of the three-dimensional quantum state carried by the photon can be maintained at around 89%.[18]

Raman scattering in solids

Diamond has very high Raman gain in optical phonon mode of 40 THz and has a wide transient window in a visible and near-infrared band, which makes it suitable for being an optical memory with a very wide band. After the Raman storage interaction, the optical phonon decays into a pair of photons through the channel, and the decay lifetime is 3.5 ps, which makes the diamond memory unsuitable for communication protocol.

Nevertheless, diamond memory has allowed some revealing studies of the interactions between light and matter at the quantum level: optical phonons in a diamond can be used to demonstrate emission quantum memory, macroscopic entanglement, pre-predicted single-photon storage, and single-photon frequency manipulation.[19]

Future development

For quantum memory, quantum communication and cryptography are the future research directions. However, there are many challenges to building a global quantum network. One of the most important challenges is to create memories that can store the quantum information carried by light. Researchers at the University of Geneva in Switzerland working with France's CNRS have discovered a new material in which an element called ytterbium can store and protect quantum information, even at high frequencies. This makes ytterbium an ideal candidate for future quantum networks. Because signals cannot be replicated, scientists are now studying how quantum memories can be made to travel farther and farther by capturing photons to synchronize them. In order to do this, it becomes important to find the right materials for making quantum memories. Ytterbium is a good insulator and works at high frequencies so that photons can be stored and quickly restored.

See also

References

  1. Tittel, Wolfgang; Sanders, Barry C.; Lvovsky, Alexander I. (December 2009). "Optical quantum memory". Nature Photonics. 3 (12): 706–714. Bibcode:2009NaPho...3..706L. doi:10.1038/nphoton.2009.231. ISSN 1749-4893.
  2. Gouët, Jean-Louis Le; Moiseev, Sergey (2012). "Quantum Memory". Journal of Physics B: Atomic, Molecular and Optical Physics. 45 (12): 120201. doi:10.1088/0953-4075/45/12/120201.
  3. Ohlsson, Nicklas; Kröll, Stefan; Moiseev, Serguei A. (2003). Bigelow, N. P.; Eberly, J. H.; Stroud, C. R.; Walmsley, I. A. (eds.). "Delayed single-photon self-interference — A double slit experiment in the time domain". Coherence and Quantum Optics VIII. Springer US: 383–384. doi:10.1007/978-1-4419-8907-9_80. ISBN 9781441989079.
  4. "Quantum Memory". photonics.anu.edu.au. Retrieved 2020-06-18.
  5. Freer, S.; Simmons, S.; Laucht, A.; Muhonen, J. T.; Dehollain, J. P.; Kalra, R.; Mohiyaddin, F. A.; Hudson, F.; Itoh, K. M.; McCallum, J. C.; Jamieson, D. N.; Dzurak, A. S.; Morello, A. (2016). "A single-atom quantum memory in silicon". Quantum Science and Technology. 2: 015009. arXiv:1608.07109. doi:10.1088/2058-9565/aa63a4.
  6. "Shengwang Du Group | Atom and Quantum Optics Lab". Retrieved 2019-05-12.
  7. "RC02_William Mong Institute of Nano Science and Technology | Institutes and Centers | Research Institutes and Centers | Research | HKUST Department of Physics". physics.ust.hk. Retrieved 2019-05-12.
  8. "Quantum memories [GAP-Optique]". www.unige.ch. Retrieved 2019-05-12.
  9. Tittel, W.; Afzelius, M.; Chaneliére, T.; Cone, R. L.; Kröll, S.; Moiseev, S. A.; Sellars, M. (2010). "Photon-echo quantum memory in solid state systems". Laser & Photonics Reviews. 4 (2): 244–267. Bibcode:2010LPRv....4..244T. doi:10.1002/lpor.200810056. ISSN 1863-8899.
  10. "Quantum Communication | PicoQuant". www.picoquant.com. Retrieved 2019-05-12.
  11. Heshami, Khabat; England, Duncan G.; Humphreys, Peter C.; Bustard, Philip J.; Acosta, Victor M.; Nunn, Joshua; Sussman, Benjamin J. (2016-11-12). "Quantum memories: emerging applications and recent advances". Journal of Modern Optics. 63 (20): 2005–2028. doi:10.1080/09500340.2016.1148212. ISSN 0950-0340. PMC 5020357. PMID 27695198.
  12. Heshami, Khabat; England, Duncan G.; Humphreys, Peter C.; Bustard, Philip J.; Acosta, Victor M.; Nunn, Joshua; Sussman, Benjamin J. (2016-11-12). "Quantum memories: emerging applications and recent advances". Journal of Modern Optics. 63 (20): 2005–2028. doi:10.1080/09500340.2016.1148212. ISSN 0950-0340. PMC 5020357. PMID 27695198.
  13. "Quantum Memory". photonics.anu.edu.au. Retrieved 2019-05-12.
  14. Harris, S. E.; Field, J. E.; Imamoğlu, A. (5 March 1990). "Nonlinear optical processes using electromagnetically induced transparency". Physical Review Letters. American Physical Society (APS). 64 (10): 1107–1110. Bibcode:1990PhRvL..64.1107H. doi:10.1103/physrevlett.64.1107. ISSN 0031-9007. PMID 10041301.
  15. Ma, Lijun; Slattery, Oliver; Tang, Xiao (April 2017). "Optical quantum memory based on electromagnetically induced transparency". Journal of Optics. 19 (4): 043001. Bibcode:2017JOpt...19d3001M. doi:10.1088/2040-8986/19/4/043001. ISSN 2040-8978. PMC 5562294. PMID 28828172.
  16. Hsiao, Ya-Fen; Tsai, Pin-Ju; Chen, Hung-Shiue; Lin, Sheng-Xiang; Hung, Chih-Chiao; Lee, Chih-Hsi; Chen, Yi-Hsin; Chen, Yong-Fan; Yu, Ite A.; Chen, IYing-Cheng (May 2018). "Highly Efficient Coherent Optical Memory Based on Electromagnetically Induced Transparency". Phys. Rev. Lett. 120 (18): 183602. arXiv:1605.08519. Bibcode:2018PhRvL.120r3602H. doi:10.1103/PhysRevLett.120.183602. PMID 29775362.
  17. "Solid State Quantum Memories | QPSA @ ICFO". qpsa.icfo.es. Retrieved 2019-05-12.
  18. Simon, C.; Afzelius, M.; Appel, J.; Boyer de la Giroday, A.; Dewhurst, S. J.; Gisin, N.; Hu, C. Y.; Jelezko, F.; Kröll, S. (2010-05-01). "Quantum memories". The European Physical Journal D. 58 (1): 1–22. arXiv:1003.1107. doi:10.1140/epjd/e2010-00103-y. ISSN 1434-6079.
  19. Heshami, Khabat; England, Duncan G.; Humphreys, Peter C.; Bustard, Philip J.; Acosta, Victor M.; Nunn, Joshua; Sussman, Benjamin J. (2016-11-12). "Quantum memories: emerging applications and recent advances". Journal of Modern Optics. 63 (20): 2005–2028. doi:10.1080/09500340.2016.1148212. ISSN 0950-0340. PMC 5020357. PMID 27695198.
This article is issued from Wikipedia. The text is licensed under Creative Commons - Attribution - Sharealike. Additional terms may apply for the media files.