Atom optics

Last updated

Atom optics (or atomic optics) "refers to techniques to manipulate the trajectories and exploit the wave properties of neutral atoms". [1] Typical experiments employ beams of cold, slowly moving neutral atoms, as a special case of a particle beam. Like an optical beam, the atomic beam may exhibit diffraction and interference, and can be focused with a Fresnel zone plate [2] or a concave atomic mirror. [3]

Contents

For comprehensive overviews of atom optics, see the 1994 review by Adams, Sigel, and Mlynek [1] or the 2009 review by Cronin, Jörg, and Pritchard. [4] More bibliography about Atom Optics can be found in the 2017 Resource Letter in the American Journal of Physics. [5] For quantum atom optics see the 2018 review by Pezzè et al. [6]

History

Interference of atom matter waves was first observed by Esterman and Stern in 1930, when a Na beam was diffracted off a surface of NaCl. [7] The short de Broglie wavelength of atoms prevented progress for many years until two technological breakthroughs revived interest: microlithography allowing precise small devices and laser cooling allowing atoms to be slowed, increasing their de Broglie wavelength. [1]

Until 2006, the resolution of imaging systems based on atomic beams was not better than that of an optical microscope, mainly due to the poor performance of the focusing elements. Such elements use small numerical aperture; usually, atomic mirrors use grazing incidence, and the reflectivity drops drastically with increase of the grazing angle; for efficient normal reflection, atoms should be ultracold, and dealing with such atoms usually involves magnetic, magneto-optical or optical traps.

At the beginning of the 21st century scientific publications about "atom nano-optics", evanescent field lenses [8] and ridged mirrors [9] [10] showed significant improvement. [11] In particular, an atomic hologram can be realized. [12]

See also

Related Research Articles

<span class="mw-page-title-main">Laser cooling</span> Class of methods for cooling atoms to very low temperatures

Laser cooling includes a number of techniques where atoms, molecules, and small mechanical systems are cooled with laser light. The directed energy of lasers is often associated with heating materials, e.g. laser cutting, so it can be counterintuitive that laser cooling often results in sample temperatures approaching absolute zero. Laser cooling relies on the change in momentum when an object, such as an atom, absorbs and re-emits a photon. For example, if laser light illuminates a warm cloud of atoms from all directions and the laser's frequency is tuned below an atomic resonance, the atoms will be cooled. This common type of laser cooling relies on the Doppler effect where individual atoms will preferentially absorb laser light from the direction opposite to the atom's motion. The absorbed light is re-emitted by the atom in a random direction. After repeated emission and absorption of light the net effect on the cloud of atoms is that they will expand more slowly. The slower expansion reflects a decrease in the velocity distribution of the atoms, which corresponds to a lower temperature and therefore the atoms have been cooled. For an ensemble of particles, their thermodynamic temperature is proportional to the variance in their velocity. More homogeneous velocities between particles corresponds to a lower temperature. Laser cooling techniques combine atomic spectroscopy with the aforementioned mechanical effect of light to compress the velocity distribution of an ensemble of particles, thereby cooling the particles.

Matter waves are a central part of the theory of quantum mechanics, being half of wave–particle duality. All matter exhibits wave-like behavior. For example, a beam of electrons can be diffracted just like a beam of light or a water wave.

<span class="mw-page-title-main">Quantum Zeno effect</span> Quantum measurement phenomenon

The quantum Zeno effect is a feature of quantum-mechanical systems allowing a particle's time evolution to be slowed down by measuring it frequently enough with respect to some chosen measurement setting.

An atom interferometer is an interferometer which uses the wave character of atoms. Similar to optical interferometers, atom interferometers measure the difference in phase between atomic matter waves along different paths. Today, atomic interference is typically controlled with laser beams. Atom interferometers have many uses in fundamental physics including measurements of the gravitational constant, the fine-structure constant, the universality of free fall, and have been proposed as a method to detect gravitational waves. They also have applied uses as accelerometers, rotation sensors, and gravity gradiometers.

Atomic coherence is the induced coherence between levels of a multi-level atomic system.

<span class="mw-page-title-main">Optical microcavity</span>

An optical microcavity or microresonator is a structure formed by reflecting faces on the two sides of a spacer layer or optical medium, or by wrapping a waveguide in a circular fashion to form a ring. The former type is a standing wave cavity, and the latter is a traveling wave cavity. The name microcavity stems from the fact that it is often only a few micrometers thick, the spacer layer sometimes even in the nanometer range. As with common lasers, this forms an optical cavity or optical resonator, allowing a standing wave to form inside the spacer layer or a traveling wave that goes around in the ring.

An atom laser is a coherent state of propagating atoms. They are created out of a Bose–Einstein condensate of atoms that are output coupled using various techniques. Much like an optical laser, an atom laser is a coherent beam that behaves like a wave. There has been some argument that the term "atom laser" is misleading. Indeed, "laser" stands for light amplification by stimulated emission of radiation which is not particularly related to the physical object called an atom laser, and perhaps describes more accurately the Bose–Einstein condensate (BEC). The terminology most widely used in the community today is to distinguish between the BEC, typically obtained by evaporation in a conservative trap, from the atom laser itself, which is a propagating atomic wave obtained by extraction from a previously realized BEC. Some ongoing experimental research tries to obtain directly an atom laser from a "hot" beam of atoms without making a trapped BEC first.

In physics, an atomic mirror is a device which reflects neutral atoms in a way similar to the way a conventional mirror reflects visible light. Atomic mirrors can be made of electric fields or magnetic fields, electromagnetic waves or just silicon wafer; in the last case, atoms are reflected by the attracting tails of the van der Waals attraction. Such reflection is efficient when the normal component of the wavenumber of the atoms is small or comparable to the effective depth of the attraction potential. To reduce the normal component, most atomic mirrors are blazed at the grazing incidence.

In atomic physics, a ridged mirror is a kind of atomic mirror, designed for the specular reflection of neutral particles (atoms) coming at a grazing incidence angle. In order to reduce the mean attraction of particles to the surface and increase the reflectivity, this surface has narrow ridges.

Quantum reflection is a uniquely quantum phenomenon in which an object, such as a neutron or a small molecule, reflects smoothly and in a wavelike fashion from a much larger surface, such as a pool of mercury. A classically behaving neutron or molecule will strike the same surface much like a thrown ball, hitting only at one atomic-scale location where it is either absorbed or scattered. Quantum reflection provides a powerful experimental demonstration of particle-wave duality, since it is the extended quantum wave packet of the particle, rather than the particle itself, that reflects from the larger surface. It is similar to reflection high-energy electron diffraction, where electrons reflect and diffraction from surfaces, and grazing incidence atom scattering, where the fact that atoms can also be waves is used to diffract from surfaces.

The Institute for Laser Science is a department of the University of Electro Communications, located near Tokyo, Japan.

Interferometric microscopy or imaging interferometric microscopy is the concept of microscopy which is related to holography, synthetic-aperture imaging, and off-axis-dark-field illumination techniques. Interferometric microscopy allows enhancement of resolution of optical microscopy due to interferometric (holographic) registration of several partial images and the numerical combining.

Within quantum technology, a quantum sensor utilizes properties of quantum mechanics, such as quantum entanglement, quantum interference, and quantum state squeezing, which have optimized precision and beat current limits in sensor technology. The field of quantum sensing deals with the design and engineering of quantum sources and quantum measurements that are able to beat the performance of any classical strategy in a number of technological applications. This can be done with photonic systems or solid state systems.

<span class="mw-page-title-main">Talbot effect</span> Near-field diffraction effect

The Talbot effect is a diffraction effect first observed in 1836 by Henry Fox Talbot. When a plane wave is incident upon a periodic diffraction grating, the image of the grating is repeated at regular distances away from the grating plane. The regular distance is called the Talbot length, and the repeated images are called self images or Talbot images. Furthermore, at half the Talbot length, a self-image also occurs, but phase-shifted by half a period. At smaller regular fractions of the Talbot length, sub-images can also be observed. At one quarter of the Talbot length, the self-image is halved in size, and appears with half the period of the grating. At one eighth of the Talbot length, the period and size of the images is halved again, and so forth creating a fractal pattern of sub images with ever-decreasing size, often referred to as a Talbot carpet. Talbot cavities are used for coherent beam combination of laser sets.

Diffraction in time is a phenomenon associated with the quantum dynamics of suddenly released matter waves initially confined in a region of space. It was introduced in 1952 by Marcos Moshinsky with the shutter problem. A matter-wave beam stopped by an absorbing shutter exhibits an oscillatory density profile during its propagation after removal of the shutter. Whenever this propagation is accurately described by the time-dependent Schrödinger equation, the transient wave functions resemble the solutions that appear for the intensity of light subject to Fresnel diffraction by a straight edge. For this reason, the transient phenomenon was dubbed diffraction in time and has since then been recognised as ubiquitous in quantum dynamics. The experimental confirmation of this phenomenon was only achieved about half a century later in the group of ultracold atoms directed by Jean Dalibard.

Victor Ivanovich Balykin is a Russian physicist whose main contributions are in the field of atom optics. He and his associates first demonstrated laser cooling of neutral atoms in 1981.

Quantum microscopy allows microscopic properties of matter and quantum particles to be measured and imaged. Various types of microscopy use quantum principles. The first microscope to do so was the scanning tunneling microscope, which paved the way for development of the photoionization microscope and the quantum entanglement microscope.

<span class="mw-page-title-main">Crispin Gardiner</span> New Zealand physicist (born 1942)

Crispin William Gardiner is a New Zealand physicist, who has worked in the fields of quantum optics, ultracold atoms and stochastic processes. He has written about 120 journal articles and several books in the fields of quantum optics, stochastic processes and ultracold atoms.

<span class="mw-page-title-main">Carlos Stroud</span> American physicist

Carlos Ray Stroud, Jr. is an American physicist and educator. Working in the field of quantum optics, Stroud has carried out theoretical and experimental studies in most areas of the field from its beginnings in the late 1960s, studying the fundamentals of the quantum mechanics of atoms and light and their interaction. He has authored over 140 peer-reviewed papers and edited seven books. He is a fellow of the American Physical Society and the Optical Society of America, as well as a Distinguished Traveling Lecturer of the Division of Laser Science of the American Physical Society. In this latter position he travels to smaller colleges giving colloquia and public lectures.

Bruce W. Shore was an American theoretical physicist known for his works in atomic physics and the theory of the interaction of light with matter.

References

  1. 1 2 3 Adams, C.S; Sigel, M; Mlynek, J (1994). "Atom optics". Physics Reports. Elsevier BV. 240 (3): 143–210. doi: 10.1016/0370-1573(94)90066-3 . ISSN   0370-1573.
  2. R.B.Doak; R.E.Grisenti; S.Rehbein; G.Schmahl; J.P.Toennies; Ch. Wöll (1999). "Towards Realization of an Atomic de Broglie Microscope: Helium Atom Focusing Using Fresnel Zone Plates" (PDF). Physical Review Letters . 83 (21): 4229–4232. Bibcode:1999PhRvL..83.4229D. doi:10.1103/PhysRevLett.83.4229. Archived from the original (PDF) on 2011-09-29. Retrieved 12 March 2024.
  3. J.J.Berkhout; O.J.Luiten; I.D.Setija; T.W.Hijmans; T.Mizusaki; J.T.M.Walraven (1989). "Quantum reflection: Focusing of hydrogen atoms with a concave mirror" (PDF). Physical Review Letters . 63 (16): 1689–1692. Bibcode:1989PhRvL..63.1689B. doi:10.1103/PhysRevLett.63.1689. PMID   10040645.
  4. Cronin, Alexander D.; Jörg Schmiedmayer; David E. Pritchard (2009). "Optics and interferometry with atoms and molecules" (PDF). Reviews of Modern Physics . 81 (3): 1051. arXiv: 0712.3703 . Bibcode:2009RvMP...81.1051C. doi:10.1103/RevModPhys.81.1051. hdl:1721.1/52372. S2CID   28009912. Archived from the original (PDF) on 2011-07-19.
  5. Rohwedder, B. (2007). "Resource Letter AON-1: Atom optics, a tool for nanofabrication". American Journal of Physics. 75 (5): 394–406. Bibcode:2007AmJPh..75..394R. doi:10.1119/1.2673209.
  6. Pezzè, Luca; Smerzi, Augusto; Oberthaler, Markus K.; Schmied, Roman; Treutlein, Philipp (2018-09-05). "Quantum metrology with nonclassical states of atomic ensembles". Reviews of Modern Physics. American Physical Society (APS). 90 (3): 035005. arXiv: 1609.01609 . doi:10.1103/revmodphys.90.035005. ISSN   0034-6861. S2CID   119250709.
  7. Estermann, I.; Stern, Otto (1930). "Beugung von Molekularstrahlen". Z. Phys. 61 (1–2): 95. Bibcode:1930ZPhy...61...95E. doi:10.1007/bf01340293. S2CID   121757478.
  8. Balykin, Victor; Klimov, Vasili; Letokhov, Vlasilen (March 2005). "Atom Nano-Optics". Optics and Photonics News : 44–48.
  9. H.Oberst; D.Kouznetsov; K.Shimizu; J.Fujita; F. Shimizu (2005). "Fresnel Diffraction Mirror for an Atomic Wave". Physical Review Letters . 94 (1): 013203. Bibcode:2005PhRvL..94a3203O. doi:10.1103/PhysRevLett.94.013203. hdl: 2241/104208 . PMID   15698079.
  10. D.Kouznetsov; H. Oberst; K. Shimizu; A. Neumann; Y. Kuznetsova; J.-F. Bisson; K. Ueda; S. R. J. Brueck (2006). "Ridged atomic mirrors and atomic nanoscope". Journal of Physics B . 39 (7): 1605–1623. Bibcode:2006JPhB...39.1605K. CiteSeerX   10.1.1.172.7872 . doi:10.1088/0953-4075/39/7/005. S2CID   16653364.
  11. F, Schmidt-Kaler; T Pfau; P Schmelcher; W Schleich (2010). "Focus on Atom Optics and its Applications". New Journal of Physics . 12 (6): 065014. Bibcode:2010NJPh...12f5014S. doi: 10.1088/1367-2630/12/6/065014 .
  12. Shimizu; J. Fujita (2002). "Reflection-Type Hologram for Atoms". Physical Review Letters . 88 (12): 123201. Bibcode:2002PhRvL..88l3201S. doi:10.1103/PhysRevLett.88.123201. PMID   11909457.

Books