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  • Vol. 18, Iss. 23 — Dec. 1, 1993
  • pp: 2041–2043

Chronocyclic tomography for measuring the amplitude and phase structure of optical pulses

M. Beck, M. G. Raymer, I. A. Walmsley, and V. Wong  »View Author Affiliations


Optics Letters, Vol. 18, Issue 23, pp. 2041-2043 (1993)
http://dx.doi.org/10.1364/OL.18.002041


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Abstract

We describe a new method—chronocyclic tomography—for determining the amplitude and phase structure of a short optical pulse. The technique is based on measurements of the energy spectrum of the pulse after it has passed through a time–frequency-domain imaging system. Tomographic inversion of these measured spectra yields the time–frequency Wigner distribution of the pulse, which uniquely determines the amplitude and phase structure.

© 1993 Optical Society of America

History
Original Manuscript: July 13, 1993
Published: December 1, 1993

Citation
M. Beck, I. A. Walmsley, V. Wong, and M. G. Raymer, "Chronocyclic tomography for measuring the amplitude and phase structure of optical pulses," Opt. Lett. 18, 2041-2043 (1993)
http://www.opticsinfobase.org/ol/abstract.cfm?URI=ol-18-23-2041


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References

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  11. All Fourier-transform pairs will be represented by f˜(ω)=(2π)−1/2∫−∞∞f(t)exp(iωt)dt,where ω denotes the frequency as measured from some average carrier frequencyω¯. All times t and frequencies ω will be dimensionless quantities (i.e., scaled by a characteristic time T).
  12. Our definition differs from that of Ref. 9 (see Ref. 13).
  13. D. T. Smithy, M. Beck, A. Faridani, M. G. Raymer, Phys. Rev. Lett. 70, 1244 (1993). [CrossRef]
  14. G. T. Herman, Image Reconstruction from Projections: The Fundamentals of Computerized Tomography (Academic, New York, 1980), Chaps. 6–8, p. 90.
  15. The probability distributions are normalized such that ∫−∞∞Pθ(ωθ)dωθ=1.

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