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Three - University of Arkansas Physics Department

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Experimental observation <strong>of</strong> chirped continuous<br />

pulse-tr ain soliton solutions to the Maxwell-<br />

Bloch equations<br />

Shihadeh M. Saadeh, John L. Shultz, and Gregory J. Salamo<br />

<strong>Department</strong> <strong>of</strong> <strong>Physics</strong>, <strong>University</strong> <strong>of</strong> <strong>Arkansas</strong>, Fayetteville, <strong>Arkansas</strong>, USA<br />

Abstract: A frequency chirped continuous wave laser beam incident upon a<br />

resonant, two-level atomic absorber is seen to evolve into a Jacobi ellipticpulsetrain<br />

solution to the Maxwell-Bloch equations. Experimental pulse-train<br />

envelopes are found in good agreement with numerical and analytical<br />

predictions.<br />

02000 Optical Society <strong>of</strong> America<br />

OCIS codes: (190.5530) Pulse propagation and solitons, (190.5940) Self-action effects<br />

References and links<br />

I. S. L. McCall and E. L. Hahn, "Self-induced transparency," Phys. Rev. 183,457-485 (1969).<br />

2. J. H. Eberly, "Optical pulse and pulse-train propagation in a resonant medium," Phys. Rev. Lett. 22, 760-762<br />

(1969).<br />

3. M. D. Crisp, "Distortionless propagation <strong>of</strong> light through an optical medium," Phys. Rev. Lett. 22, 820-823<br />

(1969).<br />

4. D. Dialetis, "Propagation <strong>of</strong> electromagnetic radiation through a resonant medium," Phys. Rev. A 2, 1065.1075<br />

(1970).<br />

5. L. Matulic and J. H. Eberly, "Analytic study <strong>of</strong> pulse chirping in self-induced transparency," Phys. Rev. A 6,<br />

822-836 (1972).<br />

6. M. A. Newbold and G. J. Salamo, "Effects <strong>of</strong> relaxation on coherent continuous-pulse-train propagation," Phys.<br />

Rev. Lett. 42, 887-890 (1979).<br />

7. J. L. Shultz and G. J. Salamo, "Experimental observation <strong>of</strong> the continuous pulse-train soliton solution to the<br />

Maxwell-Bloch equations," Phys. Rev. Lett. 78, 855-858 (1997).<br />

8. N. Akhmediev and J. M. Soto-Crespo, "Dynamics <strong>of</strong> solitonlike pulse propagation in birefringent optical fibers,"<br />

Phys. Rev. E 49,5742-5754 (1994).<br />

Coherent propagation <strong>of</strong> trains <strong>of</strong> optical pulses through atwo-level absorber has beeninvestigated,<br />

from a theoretical viewpoint, by many researchers. These investigations have been based on the<br />

self-induced transparency (SIT) equations [I], both with [2-51, and without [6], the assumption <strong>of</strong><br />

zero relaxation. Recently, theoretical predictions have been supported by experimental<br />

observations <strong>of</strong> the Jacobi elliptic dn solution [7]. In particular, experiments demonstrated the<br />

evolution <strong>of</strong> an arbitrarily shaped input optical pulse train into the analytic shape-preserving Jacobi<br />

elliptic pulse train solution to the Maxwell-Bloch equations [8]. A special feature <strong>of</strong> the observed<br />

solution was that the chirp in the optical frequency <strong>of</strong> the pulse train was zero. In this paper we<br />

report the experimental and numerical demonstration <strong>of</strong> the evolution <strong>of</strong> a continuous wave laser<br />

beam into an analytic shape-preserving pulse train solution. In this case, the analytic solution to<br />

the Maxwell-Bloch equations is a Jacobi elliptic function with a nonzero frequency chirp.<br />

The interaction <strong>of</strong> a plane-wave optical field with an inhomogeneously broadened two-level<br />

absorber can be described by two sets <strong>of</strong> equations. The Bloch equations describe the effect <strong>of</strong> the<br />

optical field on the atom while the reduced Maxwell equations describe the effect <strong>of</strong> the atom on<br />

the optical field. For significant absorption, self-consistent solutions to both equations describe the<br />

propagation <strong>of</strong> the optical field through the two-level absorber. Together, the two sets <strong>of</strong> equations<br />

are known as the reduced Maxwell-Bloch equations.<br />

For circularly polarized light traveling in the z-direction, the electric field at the position <strong>of</strong> the<br />

#29439 - $15.00 US<br />

(C) 200 1 OSA<br />

Received November 22,2000; Revised January 10,2001<br />

15 January 2001 1 Vol. 8, No. 2 1 OPTICS EXPRESS 153

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