(Redirected from Solitons)In
mathematics and
physics, a 'soliton' is a self-reinforcing solitary wave (a wave packet or pulse) that maintains its shape while it travels at constant speed; solitons are caused by a delicate balance between
nonlinear and dispersive effects in the medium. ("Dispersive effects" refer to a relationship between the frequency and the speed of waves in the medium.) Solitons are found in many physical phenomena, as they arise as the solutions of a widespread class of weakly nonlinear dispersive
partial differential equations describing physical systems. The soliton phenomenon was first described by
John Scott Russell (1808–1882) who observed a solitary wave in the
Union Canal (a canal in Scotland), reproduced the phenomenon in a wave tank, and named it the "
Wave of Translation".
It is not easy to define precisely what a soliton is. Drazin and Johnson (1989) describe solitons as solutions of nonlinear differential equations which
# represent waves of permanent form;
# are localised, so that they decay or approach a constant at infinity;
# can interact strongly with other solitons, but they emerge from the collision unchanged apart from a
phase shift.
More formal definitions exist, but they require substantial mathematics. On the other hand, some scientists use the term ''soliton'' for phenomena that do not quite have these three properties (for instance, the '
light bullets' of
nonlinear optics are often called solitons despite losing energy during interaction).
To see how dispersion and non-linearity can interact to produce permanent and localized wave forms, consider a pulse of light traveling in glass. This pulse can be thought of as consisting of light of several different frequencies; since glass shows dispersion, these different frequencies will travel at different speeds and the shape of the pulse will therefore change over time. However, there is also the non-linear
Kerr effect: the speed of light of a given frequency depends on the light's amplitude or strength. If the pulse has just the right shape, the Kerr effect will exactly cancel the effect of dispersion, and the pulse's shape won't change over time: a soliton. See
soliton (optics) for a much more detailed description.
Many
exactly solvable models have soliton solutions, including the
Korteweg-de Vries equation, the
nonlinear Schrödinger equation, the coupled nonlinear Schrödinger equation, and the
sine-Gordon equation. The soliton solutions are typically obtained by means of the
inverse scattering transform. The mathematical theory of these equations is a broad and very active field of mathematical research.
Some types of
tidal bore, a wave phenomenon of a few rivers including the
River Severn, are 'undular': a wavefront followed by a train of solitons. Other solitons occur as the undersea
internal waves, initiated by seabed
topography, that propagate on the oceanic
pycnocline. Atmospheric solitons also exist, such as the
Morning Glory Cloud of the
Gulf of Carpentaria, where pressure solitons travelling in a
temperature inversion layer produce vast linear
roll clouds. The recent and not widely accepted
soliton model in
neuroscience proposes to explain the signal conduction within
neurons as pressure solitons.
In a broader sense, solitons belong to a class of phenomomena known as "
topological defects" or "topological solitons". These are a generalization of the notion of a soliton to any solution of a set of
partial differential equations that is stable against decay to the "trivial solution" due to topological constraints. The constraint arises almost always because the differential equations must obey a set of
boundary conditions, and the boundary has a non-trivial
homotopy group, preserved by the differential equations. Thus, the solutions of the differential equations can be classified into
homotopy classes. There is no continuous transformation that will map a solution in one homotopy class to another; thus the solutions are truly distinct, and maintain their integrity, even in the face of extremely powerful forces. Examples of topological solitons include the
screw dislocation in a
crystalline lattice, the
Dirac string and the
magnetic monopole in
electromagnetism, the
Skyrmion and the
Wess-Zumino-Witten model in
quantum field theory, and
cosmic strings and
domain walls in
cosmology.
History
In 1834,
John Scott Russell describes his ''
wave of translation''.
In 1965
Norman Zabusky of
Bell Labs and
Martin Kruskal of
Princeton University first demonstrated soliton behaviour in media subject to the
Korteweg-de Vries equation (KdV equation) in a computational investigation using a
finite difference approach.
In 1967, Gardner, Greene, Kruskal and Miura discovered an
inverse scattering transform enabling
analytical solution of the KdV equation. The work of
Peter Lax on
Lax pairs and the Lax equation has since extended this to solution of many related soliton-generating systems.
Solitons in fiber optics
In 1973, Akira Hasegawa of
AT&T Bell Labs was the first to suggest that solitons could exist in
optical fibers, due to a balance between
self-phase modulation and
anomalous dispersion. He also proposed the idea of a soliton-based transmission system to increase performance of optical
telecommunications.
Solitons in a fiber optic system are described by the
Manakov equations.
In 1987, P. Emplit, J.P. Hamaide, F. Reynaud, C. Froehly and A. Barthelemy, from the Universities of Brussels and Limoges, made the first experimental observation of the propagation of a
dark soliton, in an optical fiber.
In 1988, Linn Mollenauer and his team transmitted soliton pulses over 4,000 kilometers using a phenomenon called the
Raman effect, named for the Indian scientist
Sir C. V. Raman who first described it in the
1920s, to provide
optical gain in the fiber.
In 1991, a Bell Labs research team transmitted solitons error-free at 2.5 gigabits per second over more than 14,000 kilometers, using
erbium optical fiber amplifiers (spliced-in segments of optical fiber containing the rare earth element erbium). Pump lasers, coupled to the optical amplifiers, activate the erbium, which energizes the light pulses.
In 1998, Thierry Georges and his team at
France Télécom R&D Center, combining optical solitons of different wavelengths (
wavelength division multiplexing), demonstrated a data transmission of 1
terabit per second (1,000,000,000,000 units of information per second).
In 2001, the practical use of solitons became a reality when Algety Telecom deployed submarine
telecommunications equipment in Europe carrying real traffic using
John Scott Russell's solitary wave.
Bions
The bound state of two solitons is known as a ''bion''.
See also
★
Soliton (optics)
★
Soliton (topological).
★
Solitary waves in discrete media
[1]
★
Freak waves may be a related phenomenon.
★
Topological quantum number
★
Oscillons
★
Soliton model of nerve impulse propagation
References
★ N. J. Zabusky and M. D. Kruskal (1965). ''Interaction of 'Solitons' in a Collisionless Plasma and the Recurrence of Initial States.'' Phys Rev Lett 15, 240
★ A. Hasegawa and F. Tappert (1973). ''Transmission of stationary nonlinear optical pulses in dispersive dielectric fibers. I. Anomalous dispersion.'' Appl. Phys. Lett. Volume 23, Issue 3, pp. 142-144.
★ P. Emplit, J.P. Hamaide, F. Reynaud, C. Froehly and A. Barthelemy (1987) ''Picosecond steps and dark pulses through nonlinear single mode fibers.'' Optics. Comm. 62, 374
★ P. G. Drazin and R. S. Johnson (1989). ''Solitons: an introduction.'' Cambridge University Press.
External links
★
morningglorycloud.com has video of the Morning Glory Cloud in Australia's Gulf of Carpentaria
★
Solitons, solitary waves and secondary or baby solitary waves in discrete media
★
Heriot-Watt University soliton page
★
The many faces of solitons
★
Klaus Brauer's soliton page
★
Solitons and Soliton Collisions
★
John Scott Russell and the solitary wave
★
Severn Bore web site
★
John Scott Russell biography
★
Soliton in Electrical Engineering
★
Miura's home page
★
Photograph of Soliton on the Scott Russell Aqueduct
★
Solitons possible agent of nerve transmission (PDF)(pnas.org)