SOLITONS From Canal Water Waves to Molecular Lasers

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SOLITONS From Canal Water Waves to Molecular Lasers Hieu D. Nguyen Rowan University IEEE

SOLITONS From Canal Water Waves to Molecular Lasers Hieu D. Nguyen Rowan University IEEE Night 5 -20 -03

from SIAM News, Volume 31, Number 2, 1998 Making Waves: Solitons and Their Practical

from SIAM News, Volume 31, Number 2, 1998 Making Waves: Solitons and Their Practical Applications "A Bright Idea“ Economist (11/27/99) Vol. 353, No. 8147, P. 84 Solitons, waves that move at a constant shape and speed, can be used for fiber-optic-based data transmissions… From the Academy Mathematical frontiers in optical solitons Proceedings NAS, November 6, 2001 Number 588, May 9, 2002 Bright Solitons in a Bose-Einstein Condensate Solitons may be the wave of the future Scientists in two labs coax very cold atoms to move in trains 05/20/2002 The Dallas Morning News

Definition of ‘Soliton’ One entry found for soliton. Main Entry: sol·i·ton Pronunciation: 'sä-l&-"tän Function:

Definition of ‘Soliton’ One entry found for soliton. Main Entry: sol·i·ton Pronunciation: 'sä-l&-"tän Function: noun Etymology: solitary + 2 -on Date: 1965 : a solitary wave (as in a gaseous plasma) that propagates with little loss of energy and retains its shape and speed after colliding with another such wave http: //www. m-w. com/cgi-bin/dictionary

Solitary Waves John Scott Russell (1808 -1882) - Scottish engineer at Edinburgh - Committee

Solitary Waves John Scott Russell (1808 -1882) - Scottish engineer at Edinburgh - Committee on Waves: BAAC Union Canal at Hermiston, Scotland http: //www. ma. hw. ac. uk/~chris/scott_russell. html

Great Wave of Translation “I was observing the motion of a boat which was

Great Wave of Translation “I was observing the motion of a boat which was rapidly drawn along a narrow channel by a pair of horses, when the boat suddenly stopped - not so the mass of water in the channel which it had put in motion; it accumulated round the prow of the vessel in a state of violent agitation, then suddenly leaving it behind, rolled forward with great velocity, assuming the form of a large solitary elevation, a rounded, smooth and well-defined heap of water, which continued its course along the channel apparently without change of form or diminution of speed…” - J. Scott Russell

“…I followed it on horseback, and overtook it still rolling on at a rate

“…I followed it on horseback, and overtook it still rolling on at a rate of some eight or nine miles an hour, preserving its original figure some thirty feet long and a foot to a foot and a half in height. Its height gradually diminished, and after a chase of one or two miles I lost it in the windings of the channel. Such, in the month of August 1834, was my first chance interview with that singular and beautiful phenomenon which I have called the Wave of Translation. ” “Report on Waves” - Report of the fourteenth meeting of the British Association for the Advancement of Science, York, September 1844 (London 1845), pp 311 -390, Plates XLVII-LVII.

Copperplate etching by J. Scott Russell depicting the 30 -foot tank he built in

Copperplate etching by J. Scott Russell depicting the 30 -foot tank he built in his back garden in 1834

Controversy Over Russell’s Work 1 George Airy: - Unconvinced of the Great Wave of

Controversy Over Russell’s Work 1 George Airy: - Unconvinced of the Great Wave of Translation - Consequence of linear wave theory G. G. Stokes: - Doubted that the solitary wave could propagate without change in form Boussinesq (1871) and Rayleigh (1876); - Gave a correct nonlinear approximation theory 1 http: //www-gap. dcs. st-and. ac. uk/~history/Mathematicians/Russell_Scott. html

Model of Long Shallow Water Waves D. J. Korteweg and G. de Vries (1895)

Model of Long Shallow Water Waves D. J. Korteweg and G. de Vries (1895) - surface elevation above equilibrium - depth of water - surface tension - density of water - force due to gravity - small arbitrary constant

Korteweg-de Vries (Kd. V) Equation Rescaling: Kd. V Equation: Nonlinear Term Dispersion Term (Steepen)

Korteweg-de Vries (Kd. V) Equation Rescaling: Kd. V Equation: Nonlinear Term Dispersion Term (Steepen) (Flatten)

Stable Solutions Profile of solution curve: - Unchanging in shape - Bounded - Localized

Stable Solutions Profile of solution curve: - Unchanging in shape - Bounded - Localized Do such solutions exist? Steepen + Flatten = Stable

Solitary Wave Solutions 1. Assume traveling wave of the form: 2. Kd. V reduces

Solitary Wave Solutions 1. Assume traveling wave of the form: 2. Kd. V reduces to an integrable equation: 3. Cnoidal waves (periodic):

4. Solitary waves (one-solitons): - Assume wavelength approaches infinity

4. Solitary waves (one-solitons): - Assume wavelength approaches infinity

Other Soliton Equations Sine-Gordon Equation: - Superconductors (Josephson tunneling effect) - Relativistic field theories

Other Soliton Equations Sine-Gordon Equation: - Superconductors (Josephson tunneling effect) - Relativistic field theories Nonlinear Schroedinger (NLS) Equation: - Fiber optic transmission systems - Lasers

N-Solitons Zabusky and Kruskal (1965): - Partitions of energy modes in crystal lattices Solitary

N-Solitons Zabusky and Kruskal (1965): - Partitions of energy modes in crystal lattices Solitary waves pass through each other Coined the term ‘soliton’ (particle-like behavior) Two-soliton collision:

Inverse Scattering “Nonlinear” Fourier Transform: Space-time domain Frequency domain Fourier Series: http: //mathworld. wolfram.

Inverse Scattering “Nonlinear” Fourier Transform: Space-time domain Frequency domain Fourier Series: http: //mathworld. wolfram. com/Fourier. Series. Square. Wave. html

Solving Linear PDEs by Fourier Series 1. Heat equation: 2. Separate variables: 3. Determine

Solving Linear PDEs by Fourier Series 1. Heat equation: 2. Separate variables: 3. Determine modes: 4. Solution:

Solving Nonlinear PDEs by Inverse Scattering 1. Kd. V equation: 2. Linearize Kd. V:

Solving Nonlinear PDEs by Inverse Scattering 1. Kd. V equation: 2. Linearize Kd. V: 3. Determine spectrum: 4. Solution by inverse scattering: (discrete)

2. Linearize Kd. V

2. Linearize Kd. V

Schroedinger’s Equation (time-independent) Potential (t=0) Eigenvalue (mode) Scattering Problem: Inverse Scattering Problem: Eigenfunction

Schroedinger’s Equation (time-independent) Potential (t=0) Eigenvalue (mode) Scattering Problem: Inverse Scattering Problem: Eigenfunction

3. Determine Spectrum (a) Solve the scattering problem at t = 0 to obtain

3. Determine Spectrum (a) Solve the scattering problem at t = 0 to obtain reflection-less spectrum: (eigenvalues) (eigenfunctions) (normalizing constants) (b) Use the fact that the Kd. V equation is isospectral to obtain spectrum for all t - Lax pair {L, A}:

4. Solution by Inverse Scattering (a) Solve GLM integral equation (1955): (b) N-Solitons ([GGKM],

4. Solution by Inverse Scattering (a) Solve GLM integral equation (1955): (b) N-Solitons ([GGKM], [WT], 1970):

Soliton matrix: One-soliton (N=1): Two-solitons (N=2):

Soliton matrix: One-soliton (N=1): Two-solitons (N=2):

Unique Properties of Solitons Signature phase-shift due to collision Infinitely many conservation laws (conservation

Unique Properties of Solitons Signature phase-shift due to collision Infinitely many conservation laws (conservation of mass)

Other Methods of Solution Hirota bilinear method Backlund transformations Wronskian technique Zakharov-Shabat dressing method

Other Methods of Solution Hirota bilinear method Backlund transformations Wronskian technique Zakharov-Shabat dressing method

Decay of Solitons as particles: - Do solitons pass through or bounce off each

Decay of Solitons as particles: - Do solitons pass through or bounce off each other? Linear collision: Nonlinear collision: - Each particle decays upon collision - Exchange of particle identities - Creation of ghost particle pair

Applications of Solitons Optical Communications: - Temporal solitons (optical pulses) Lasers: - Spatial solitons

Applications of Solitons Optical Communications: - Temporal solitons (optical pulses) Lasers: - Spatial solitons (coherent beams of light) - BEC solitons (coherent beams of atoms)

Hieu Nguyen: Temporal solitons involve weak nonlinearity whereas spatial solitons involve strong nonlinearity Optical

Hieu Nguyen: Temporal solitons involve weak nonlinearity whereas spatial solitons involve strong nonlinearity Optical Phenomena Refraction Diffraction Coherent Light

NLS Equation Dispersion/diffraction term Nonlinear term One-solitons: Envelope Oscillation

NLS Equation Dispersion/diffraction term Nonlinear term One-solitons: Envelope Oscillation

Temporal Solitons (1980) Chromatic dispersion: - Pulse broadening effect Before After Self-phase modulation -

Temporal Solitons (1980) Chromatic dispersion: - Pulse broadening effect Before After Self-phase modulation - Pulse narrowing effect Before After

Spatial Solitons Diffraction - Beam broadening effect: Self-focusing intensive refraction (Kerr effect) - Beam

Spatial Solitons Diffraction - Beam broadening effect: Self-focusing intensive refraction (Kerr effect) - Beam narrowing effect

BEC (1995) Cold atoms - Coherent matter waves - Dilute alkali gases http: //cua.

BEC (1995) Cold atoms - Coherent matter waves - Dilute alkali gases http: //cua. mit. edu/ketterle_group/

Atom Lasers Atom beam: Gross-Pitaevskii equation: - Quantum field theory Atom-atom interaction External potential

Atom Lasers Atom beam: Gross-Pitaevskii equation: - Quantum field theory Atom-atom interaction External potential

Molecular Lasers Cold molecules - Bound states between two atoms (Feshbach resonance) Molecular laser

Molecular Lasers Cold molecules - Bound states between two atoms (Feshbach resonance) Molecular laser equations: (atoms) (molecules) Joint work with Hong Y. Ling (Rowan University)

Many Faces of Solitons Quantum Field Theory - Quantum solitons - Monopoles - Instantons

Many Faces of Solitons Quantum Field Theory - Quantum solitons - Monopoles - Instantons General Relativity - Bartnik-Mc. Kinnon solitons (black holes) Biochemistry - Davydov solitons (protein energy transport)

Future of Solitons "Anywhere you find waves you find solitons. " -Randall Hulet, Rice

Future of Solitons "Anywhere you find waves you find solitons. " -Randall Hulet, Rice University, on creating solitons in Bose-Einstein condensates, Dallas Morning News, May 20, 2002

Recreation of the Wave of Translation (1995) Scott Russell Aqueduct on the Union Canal

Recreation of the Wave of Translation (1995) Scott Russell Aqueduct on the Union Canal near Heriot-Watt University, 12 July 1995

References C. Gardner, J. Greene, M. Kruskal, R. Miura, Korteweg-de Vries equation and generalizations.

References C. Gardner, J. Greene, M. Kruskal, R. Miura, Korteweg-de Vries equation and generalizations. VI. Methods for exact solution, Comm. Pure and Appl. Math. 27 (1974), pp. 97 -133 R. Miura, The Korteweg-de Vries equation: a survey of results, SIAM Review 18 (1976), No. 3, 412 -459. A. Snyder and F. Ladouceur, Light Guiding Light, Optics and Photonics News, February, 1999, p. 35 P. D. Drummond, K. V. Kheruntsyan and H. He, Coherent Molecular Solitons in Bose-Einstein Condensates, Physical Review Letters 81 (1998), No. 15, 3055 -3058 B. Seaman and H. Y. Ling, Feshbach Resonance and Coherent Molecular Beam Generation in a Matter Waveguide, preprint (2003). H. D. Nguyen, Decay of Kd. V Solitons, SIAM J. Applied Math. 63 (2003), No. 3, 874 -888. M. Wadati and M. Toda, The exact N-soliton solution of the Korteweg-de Vries equation, J. Phys. Soc. Japan 32 (1972), no. 5, 1403 -1411. Solitons Home Page: http: //www. ma. hw. ac. uk/solitons/ Light Bullet Home Page: http: //people. deas. harvard. edu/~jones/solitons. html Alkali Gases @ Mit Home page: http: //cua. mit. edu/ketterle_group/ www. rowan. edu/math/nguyen/soliton/