Sine-Gordon equation

From Wikipedia, the free encyclopedia
  (Redirected from Sine–Gordon equation)
Jump to navigation Jump to search

The sine-Gordon equation is a nonlinear hyperbolic partial differential equation in 1 + 1 dimensions involving the d'Alembert operator and the sine of the unknown function. It was originally introduced by Edmond Bour (1862) in the course of study of surfaces of constant negative curvature as the Gauss–Codazzi equation for surfaces of curvature −1 in 3-space,[1] and rediscovered by Frenkel and Kontorova (1939) in their study of crystal dislocations known as the Frenkel–Kontorova model.[2] This equation attracted a lot of attention in the 1970s due to the presence of soliton solutions.

Origin of the equation and its name[edit]

There are two equivalent forms of the sine-Gordon equation. In the (real) space-time coordinates, denoted (xt), the equation reads:[3]

where partial derivatives are denoted by subscripts. Passing to the light-cone coordinates (uv), akin to asymptotic coordinates where

the equation takes the form[4]

This is the original form of the sine-Gordon equation, as it was considered in the 19th century in the course of investigation of surfaces of constant Gaussian curvature K = −1, also called pseudospherical surfaces. Choose a coordinate system for such a surface in which the coordinate mesh u = constant, v = constant is given by the asymptotic lines parameterized with respect to the arc length. The first fundamental form of the surface in these coordinates has a special form

where expresses the angle between the asymptotic lines, and for the second fundamental form, L = N = 0. Then the Codazzi–Mainardi equation expressing a compatibility condition between the first and second fundamental forms results in the sine-Gordon equation. The study of this equation and of the associated transformations of pseudospherical surfaces in the 19th century by Bianchi and Bäcklund led to the discovery of Bäcklund transformations. Another transformation of pseudospherical surfaces is the Lie transform introduced by Sophus Lie in 1879, which corresponds to Lorentz boosts in terms of light-cone coordinates, thus the sine-Gordon equation is Lorentz-invariant.[5]

The name "sine-Gordon equation" is a pun on the well-known Klein–Gordon equation in physics:[3]

The sine-Gordon equation is the Euler–Lagrange equation of the field whose Lagrangian density is given by

Using the Taylor series expansion of the cosine in the Lagrangian,

it can be rewritten as the Klein–Gordon Lagrangian plus higher-order terms:

Soliton solutions[edit]

An interesting feature of the sine-Gordon equation is the existence of soliton and multisoliton solutions.

1-soliton solutions[edit]

The sine-Gordon equation has the following 1-soliton solutions:


and the slightly more general form of the equation is assumed:

The 1-soliton solution for which we have chosen the positive root for is called a kink and represents a twist in the variable which takes the system from one solution to an adjacent with . The states are known as vacuum states, as they are constant solutions of zero energy. The 1-soliton solution in which we take the negative root for is called an antikink. The form of the 1-soliton solutions can be obtained through application of a Bäcklund transform to the trivial (constant vacuum) solution and the integration of the resulting first-order differentials:

for all time.

The 1-soliton solutions can be visualized with the use of the elastic ribbon sine-Gordon model introduced by Julio Rubinstein in 1970.[6] Here we take a clockwise (left-handed) twist of the elastic ribbon to be a kink with topological charge . The alternative counterclockwise (right-handed) twist with topological charge will be an antikink.

Traveling kink soliton represents propagating clockwise twist.[7]
Traveling antikink soliton represents propagating counterclockwise twist.[7]

2-soliton solutions[edit]

Multi-soliton solutions can be obtained through continued application of the Bäcklund transform to the 1-soliton solution, as prescribed by a Bianchi lattice relating the transformed results.[8] The 2-soliton solutions of the sine-Gordon equation show some of the characteristic features of the solitons. The traveling sine-Gordon kinks and/or antikinks pass through each other as if perfectly permeable, and the only observed effect is a phase shift. Since the colliding solitons recover their velocity and shape, such kind of interaction is called an elastic collision.

Antikink-kink collision.[7]
Kink-kink collision.[7]

Another interesting 2-soliton solutions arise from the possibility of coupled kink-antikink behaviour known as a breather. There are known three types of breathers: standing breather, traveling large-amplitude breather, and traveling small-amplitude breather.[9]

Standing breather is a swinging in time coupled kink-antikink soliton.[7]
Large-amplitude moving breather.[7]
Small-amplitude moving breather – looks exotic, but essentially has a breather envelope.[7]

3-soliton solutions[edit]

3-soliton collisions between a traveling kink and a standing breather or a traveling antikink and a standing breather results in a phase shift of the standing breather. In the process of collision between a moving kink and a standing breather, the shift of the breather is given by

where is the velocity of the kink, and is the breather's frequency.[9] If the old position of the standing breather is , after the collision the new position will be .

Collision of moving kink and standing breather.[7]
Collision of moving antikink and standing breather.[7]

FDTD (1D) video simulation of a soliton with forces[edit]

The following video shows a simulation of two parking solitons. Both send out a pressure–speed field with different polarity. Because the end of the 1D space is not terminated symmetrically, waves are reflected.

Solitons according to the sine-Gordon equation with forces

Lines in the video:

  1. cos() part of the soliton.
  2. sin() part of the soliton.
  3. Angle acceleration of the soliton.
  4. Pressure component of the field with different polarity.
  5. Speed component of the field, direction-dependent.


  1. Solitons send out not bound energy as waves.[clarify]
  2. Solitons send the pv field, which reaches the peer.
  3. Solitons begin to move.
  4. They meet in the middle and annihilate.
  5. Mass is spread as wave.

Related equations[edit]

The sinh-Gordon equation is given by[10]

This is the Euler–Lagrange equation of the Lagrangian

Another closely related equation is the elliptic sine-Gordon equation, given by

where is now a function of the variables x and y. This is no longer a soliton equation, but it has many similar properties, as it is related to the sine-Gordon equation by the analytic continuation (or Wick rotation) y = it.

The elliptic sinh-Gordon equation may be defined in a similar way.

A generalization is given by Toda field theory.[11]

Quantum version[edit]

In quantum field theory the sine-Gordon model contains a parameter that can be identified with the Planck constant. The particle spectrum consists of a soliton, an anti-soliton and a finite (possibly zero) number of breathers.[12][13][14] The number of the breathers depends on the value of the parameter. Multiparticle productions cancels on mass shell.

Semi-classical quantization of the sine-Gordon model was done by Ludwig Faddeev and Vladimir Korepin.[15] The exact quantum scattering matrix was discovered by Alexander Zamolodchikov.[16] This model is S-dual to the Thirring model.

Infinite volume and on a half line[edit]

One can also consider the sine-Gordon model on a circle,[17] on a line segment, or on a half line.[18] It is possible to find boundary conditions which preserve the integrability of the model.[18] On a half line the spectrum contains boundary bound states in addition to the solitons and breathers.[18]

Supersymmetric sine-Gordon model[edit]

A supersymmetric extension of the sine-Gordon model also exists.[19] Integrability preserving boundary conditions for this extension can be found as well.[19]

See also[edit]


  1. ^ Bour, Edmond (1862). "Theorie de la deformation des surfaces". Journal de l'École impériale polytechnique. 22 (39): 1–148. OCLC 55567842.
  2. ^ Frenkel J, Kontorova T (1939). "On the theory of plastic deformation and twinning". Izvestiya Akademii Nauk SSSR, Seriya Fizicheskaya. 1: 137–149.
  3. ^ a b Rajaraman, R. (1989). Solitons and Instantons: An Introduction to Solitons and Instantons in Quantum Field Theory. North-Holland Personal Library. Vol. 15. North-Holland. pp. 34–45. ISBN 978-0-444-87047-6.
  4. ^ Polyanin, Andrei D.; Valentin F. Zaitsev (2004). Handbook of Nonlinear Partial Differential Equations. Chapman & Hall/CRC Press. pp. 470–492. ISBN 978-1-58488-355-5.
  5. ^ Terng, C. L., & Uhlenbeck, K. (2000). "Geometry of solitons" (PDF). Notices of the AMS. 47 (1): 17–25.{{cite journal}}: CS1 maint: multiple names: authors list (link)
  6. ^ Rubinstein, Julio (1970). "Sine-Gordon equation". Journal of Mathematical Physics. 11 (1): 258–266. Bibcode:1970JMP....11..258R. doi:10.1063/1.1665057.
  7. ^ a b c d e f g h i Georgiev D. D., Papaioanou S. N., Glazebrook J. F. (2004). "Neuronic system inside neurons: molecular biology and biophysics of neuronal microtubules". Biomedical Reviews. 15: 67–75. doi:10.14748/bmr.v15.103.{{cite journal}}: CS1 maint: uses authors parameter (link)
  8. ^ Rogers, C.; W. K. Schief (2002). Bäcklund and Darboux Transformations: Geometry and Modern Applications in Soliton Theory. Cambridge Texts in Applied Mathematics. New York: Cambridge University Press. ISBN 978-0-521-01288-1.
  9. ^ a b Miroshnichenko A. E., Vasiliev A. A., Dmitriev S. V. Solitons and Soliton Collisions.
  10. ^ Polyanin, Andrei D.; Zaitsev, Valentin F. (16 December 2011). Handbook of Nonlinear Partial Differential Equations (Second ed.). Boca Raton: CRC Press. p. 485. ISBN 978-1-4200-8723-9.
  11. ^ Yuanxi, Xie; Tang, Jiashi (February 2006). "A unified method for solving sinh-Gordon–type equations". Il Nuovo Cimento B. 121 (2): 115–121. Bibcode:2006NCimB.121..115X. doi:10.1393/ncb/i2005-10164-6.
  12. ^ Korepin, V. E. (1979). "Direct calculation of the S matrix in the massive Thirring model". Theoretical and Mathematical Physics. 41 (2): 953–967. Bibcode:1979TMP....41..953K. doi:10.1007/bf01028501. S2CID 121527379.
  13. ^ Takada, Satoshi; Misawa, Susumu (1981). "The Quantum Sine-Gordon Model and the Fermi-Bose Relation". Progress of Theoretical Physics. 66 (1): 101–117. Bibcode:1981PThPh..66..101T. doi:10.1143/ptp.66.101.
  14. ^ Bogoliubov, N. M.; Korepin, V. E.; Izergin, A. G. (1985). "Structure of the vacuum in the quantum sine-Gordon model". Physics Letters B. 159 (4): 345–347. Bibcode:1985PhLB..159..345B. doi:10.1016/0370-2693(85)90264-3.
  15. ^ Faddeev, L. D.; Korepin, V. E. (1978). "Quantum theory of solitons". Physics Reports. 42 (1): 1–87. Bibcode:1978PhR....42....1F. doi:10.1016/0370-1573(78)90058-3.
  16. ^ Zamolodchikov, Alexander B.; Zamolodchikov, Alexey B. (1978). "Relativistic factorized S-matrix in two dimensions having O(N) isotopic symmetry". Nuclear Physics B. 133 (3): 525–535. Bibcode:1978NuPhB.133..525Z. doi:10.1016/0550-3213(78)90239-0.
  17. ^ McKean, H. P. (1981). "The sine-Gordon and sinh-Gordon equations on the circle". Communications on Pure and Applied Mathematics. 34 (2): 197–257. doi:10.1002/cpa.3160340204.
  18. ^ a b c Bowcock, Peter; Tzamtzis, Georgios (2007). "The complex sine-Gordon model on a half line". Journal of High Energy Physics. 2007 (3): 047. arXiv:hep-th/0203139. Bibcode:2007JHEP...03..047B. doi:10.1088/1126-6708/2007/03/047. S2CID 119501952.
  19. ^ a b Inami, Takeo; Odake, Satoru; Zhang, Yao-Zhong (1995). "Supersymmetric extension of the sine-Gordon theory with integrable boundary interactions". Physics Letters B. 359 (1): 118–124. arXiv:hep-th/9506157. Bibcode:1995PhLB..359..118I. doi:10.1016/0370-2693(95)01072-X. S2CID 18230581.

External links[edit]