Spontaneous parametric down-conversion

From Wikipedia, the free encyclopedia
Jump to: navigation, search
Spontaneous Parametric Downconversion.png

Spontaneous parametric down-conversion (also known as SPDC, parametric fluorescence, or parametric scattering) is an important process in quantum optics, used especially as a source of entangled photon pairs, and of single photons.

Basic process[edit]

An SPDC scheme with the Type I output
The video of an experiment showing vacuum fluctuations (in the red ring) amplified by SPDC (corresponding to the image above)

A nonlinear crystal is used to split photon beams into pairs of photons that, in accordance with the law of conservation of energy and law of conservation of momentum, have combined energies and momenta equal to the energy and momentum of the original photon and crystal lattice, are phase-matched in the frequency domain, and have correlated polarizations. (The state of the crystal is unchanged by the process.) The momentum conservation (by looking only on the photons) is only valid inside the crystal, which is often not clearly described in literature. If the photons would conserve momentum and energy also outside the crystal, they would have to go both to the same direction then the incoming pump photon, which can be discounted easily. So the crystal does get some momentum when the photons leave the crystal. If the photons share the same polarization it is deemed Type I correlation; if they have perpendicular polarizations it is deemed Type II. There is no polarization correlation between successive photon sets.[1]

SPDC is stimulated by random vacuum fluctuations, and hence the photon pairs are created at random times. The conversion efficiency is very low, on the order of 1 pair per 1012 incoming photons.[2] However, if one half of the pair (the "signal") is detected at any time then its partner (the "idler") is known to be present. The output of a Type I down converter is a squeezed vacuum that contains only even photon number terms. The output of the Type II down converter is a two-mode squeezed vacuum.


An SPDC scheme with the Type II output

In a commonly used SPDC apparatus design, a strong laser beam, termed the "pump" beam, is directed at a BBO (beta-barium borate) crystal. Most of the photons continue straight through the crystal. However, occasionally, some of the photons undergo spontaneous down-conversion with Type II polarization correlation, and the resultant correlated photon pairs have trajectories that are constrained to be within two cones, whose axes are symmetrically arranged relative to the pump beam. Also, due to the conservation of energy, the two photons are always symmetrically located within the cones, relative to the pump beam. Importantly, the trajectories of the photon pairs may exist simultaneously in the two lines where the cones intersect. This results in entanglement of the photon pairs whose polarization are perpendicular.[3][4]:205

Another crystal is KDP (Potassium Dihydrogen Phosphate) which is mostly used in Type I down conversion, where both photons have the same polarization.[5]


SPDC was described as early as 1970 by D. Klyshko and coauthors,[6] and D. C. Burnham and D. L. Weinberg.[7][8] It was first applied to experiments related to coherence by two independent pairs of researchers in the late 1980s: Carroll Alley and Yanhua Shih, and Rupamanjari Ghosh and Leonard Mandel.[9][10] The duality between incoherent (Van Cittert–Zernike theorem) and biphoton emissions was found.[11]


SPDC allows for the creation of optical fields containing (to a good approximation) a single photon. As of 2005, this is the predominant mechanism for experimentalists to create single photons (also known as Fock states).[12] The single photons as well as the photon pairs are often used in quantum information experiments and applications like quantum cryptography and Bell test experiments.

SPDC is widely used to create pairs of entangled photons with a high degree of spatial correlation.[13] Such pairs are used in ghost imaging, in which information is combined from two light detectors: a conventional, multi-pixel detector that doesn't view the object, and a single-pixel (bucket) detector that does view the object.


The newly observed effect of two-photon emission from electrically driven semiconductors has been proposed as a basis for more efficient sources of entangled photon pairs.[14] Other than SPDC-generated photon pairs, the photons of a semiconductor-emitted pair usually are not identical but have different energies.[15]

See also[edit]


  1. ^ Shih, Yanhua (2003). "Entangled biphoton source - property and preparation". Reports on Progress in Physics. 66 (6): 1009–1044. doi:10.1088/0034-4885/66/6/203. ISSN 0034-4885. 
  2. ^ Ling, Alexander; Lamas-Linares, Antía; Kurtsiefer, Christian (2008). "Absolute emission rates of spontaneous parametric down-conversion into single transverse Gaussian modes" (PDF). Physical Review A. 77 (4). doi:10.1103/PhysRevA.77.043834. ISSN 1050-2947. 
  3. ^ P. Kwiat; et al. (1995). "New High-Intensity Source of Polarization-Entangled Photon Pairs". Phys. Rev. Lett. 75 (24): 4337–4341. Bibcode:1995PhRvL..75.4337K. doi:10.1103/PhysRevLett.75.4337. 
  4. ^ Anton Zeilinger (12 October 2010). "The super-source and closing the communication loophole". Dance of the Photons: From Einstein to Quantum Teleportation. Farrar, Straus and Giroux. ISBN 978-1-4299-6379-4. 
  5. ^ Reck, M H A, Quantum Interferometry with Multiports: Entangled Photons in Optical Fibers (page 115) (PDF), retrieved 16 February 2014 
  6. ^ Klyshko D. N., Penin A. N., Polkovnikov B. F., "Parametric Luminescence and Light Scattering by Polaritons", JETP Lett. 11, 05 (1970)
  7. ^ D. C. Burnham and D. L. Weinberg, "Observation of simultaneity in parametric production of optical photon pairs", Phys. Rev. Lett. 25, 84 (1970)
  8. ^ D. Greenberger, M. Horne, and A. Zeilinger, "A Bell Theorem Without Inequalities for Two Particles, Using Efficient Detectors" (2005), note 18.
  9. ^ Y. Shih and C. Alley, in Proceedings of the 2nd Int'l Symposium on Foundations of QM in Light of New Technology, Namiki et al., eds., Physical Society of Japan, Tokyo, 1986.
  10. ^ R. Ghosh and L. Mandel, "Observation of Nonclassical Effects in the Interference of Two Photons", Phys. Rev. Lett. 59, 1903 (1987)
  11. ^ http://pra.aps.org/abstract/PRA/v62/i4/e043816 - Duality between partial coherence and partial entanglement
  12. ^ Zavatta, Alessandro; Viciani, Silvia; Bellini, Marco (2004). "Tomographic reconstruction of the single-photon Fock state by high-frequency homodyne detection". Physical Review A. 70 (5): 053821. arXiv:quant-ph/0406090Freely accessible. Bibcode:2004PhRvA..70e3821Z. doi:10.1103/PhysRevA.70.053821. 
  13. ^ Walborn, S.P.; Monken, C.H.; Pádua, S.; Souto Ribeiro, P.H. (2010). "Spatial correlations in parametric down-conversion" (PDF). Physics Reports. 495 (4-5): 87–139. doi:10.1016/j.physrep.2010.06.003. ISSN 0370-1573. 
  14. ^ A. Hayat, P. Ginzburg, M. Orenstein, Observation of Two-Photon Emission from Semiconductors, Nature Photon. 2, 238 (2008)
  15. ^ Chluba, J.; Sunyaev, R. A. (2006). "Induced two-photon decay of the 2s level and the rate of cosmological hydrogen recombination". Astronomy and Astrophysics. 446: 39. arXiv:astro-ph/0508144Freely accessible. Bibcode:2006A&A...446...39C. doi:10.1051/0004-6361:20053988.