Physical Review A · 1997 · 321 citations · 43 references
Natural SciencesMaterials SciencePhysicsOptical MaterialsOpticsPhotonicsElectromagnetic WavesNonlinear Optical MaterialsNonlinear OpticsPeriodic Electromagnetic StructuresPhotonic MaterialsUltrafast OpticsHarmonic GenerationNonlinear PhotonicsPhase LockingPhotonic Band GapPhotonic Band StructureSecond-harmonic GenerationUltra-short Pulse GenerationUltrashort Pulse Generation
The work is relevant to high‑energy lasers, Raman‑type sources, and frequency up‑ and down‑conversion schemes. The study numerically investigates second‑harmonic generation in a one‑dimensional photonic band‑gap material doped with a χ^(2) medium. The structure is engineered so that the pump pulse is tuned near the first‑order photonic band edge and the SH signal near the second‑order gap, exploiting high mode density, low group velocity, and spatial phase locking to enhance SH generation. Simulations show that a 20‑period, 12‑µm structure produces SH pulses with energy and power 2–3 orders of magnitude higher than a phase‑matched bulk medium, effectively enhancing the χ^(2) response and enabling mm‑ or cm‑long quasi‑phase‑matched devices to be replaced by micrometer‑scale layered structures.
We present a numerical study of second-harmonic (SH) generation in a one-dimensional, generic, photonic band-gap material that is doped with a nonlinear ${\ensuremath{\chi}}^{(2)}$ medium. We show that a 20-period, 12-\ensuremath{\mu}m structure can generate short SH pulses (similar in duration to pump pulses) whose energy and power levels may be 2--3 orders of magnitude larger than the energy and power levels produced by an equivalent length of a phase-matched, bulk medium. This phenomenon comes about as a result of the combination of high electromagnetic mode density of states, low group velocity, and spatial phase locking of the fields near the photonic band edge. The structure is designed so that the pump pulse is tuned near the first-order photonic band edge, and the SH signal is generated near the band edge of the second-order gap. This maximizes the density of available field modes for both the pump and SH field. Our results show that the ${\ensuremath{\chi}}^{(2)}$ response is effectively enhanced by several orders of magnitude. Therefore, mm- or cm-long, quasi-phase-matched devices could be replaced by these simple layered structures of only a few micrometers in length. This has important applications to high-energy lasers, Raman-type sources, and frequency up- and down-conversion schemes.
43
Resonance Absorption by Nuclear Magnetic Moments in a Solid
Edward M. Purcell, H. C. Torrey, R. V. Pound · Physical Review · 1946 · 5.9K citations · Full text
Natural Sciences, Chemistry, Physics +10
Benjamin J. Eggleton, R. E. Slusher, C. Martijn de Sterke et al. · Physical Review Letters · 1996 · 676 citations
Natural Sciences, Physics, Optics +16
The photonic band edge laser: A new approach to gain enhancement
Jonathan P. Dowling, Michael Scalora, Mark J. Bloemer et al. · Journal of Applied Physics · 1994 · 626 citations