Complete modulational-instability gain spectrum of nonlinear quasi-phase-matching gratings

We consider plane waves propagating in quadratic nonlinear slab waveguides with nonlinear quasi-phase-matching gratings. We predict analytically and verify numerically the complete gain spectrum for transverse modulational instability, including hitherto undescribed higher-order gain bands. (C) 2004 Optical Society of America.

Power-controlled phase-matching and instability of CW propagation in multicore optical fibers with a central core

We present modulation instability analysis including azimuthal perturbations of steady-state continuous wave (CW) propagation in multicore-fiber configurations with a central core. In systems with a central core, a steady CW evolution regime requires power-controlled phase matching, which offers interesting spatial-division applications. Our results have general applicability and are relevant to a range of physical and engineering systems, including high-power fiber lasers, optical transmission in multicore fiber, and systems of coupled nonlinear waveguides. © 2013 Optical Society of America.

Two-dimensional infrared spectroscopy of peptides by phase-controlled femtosecond vibrational photon echoes

Two-dimensional infrared spectra of peptides are introduced that are the direct analogues of two- and three-pulse multiple quantum NMR. Phase matching and heterodyning are used to isolate the phase and amplitudes of the electric fields of vibrational photon echoes as a function of multiple pulse delays. Structural information is made available on the time scale of a few picoseconds. Line narrowed spectra of acyl-proline-NH2 and cross peaks implying the coupling between its amide-I modes are obtained, as are the phases of the various contributions to the signals. Solvent-sensitive structural differences are seen for the dipeptide. The methods show great promise to measure structure changes in biology on a wide range of time scales.

Modulational Instability in Periodic Quadratic Nonlinear Materials

We investigate the modulational instability of plane waves in quadratic nonlinear materials with linear and nonlinear quasi-phase-matching gratings. Exact Floquet calculations, confirmed by numerical simulations, show that the periodicity can drastically alter the gain spectrum but never completely removes the instability. The low-frequency part of the gain spectrum is accurately predicted by an averaged theory and disappears for certain gratings. The high-frequency part is related to the inherent gain of the homogeneous non-phase-matched material and is a consistent spectral feature.

Sensitive detection of nitric oxide using seeded parametric four-wave mixing

A sensitive near-resonant four-wave mixing technique based on two-photon parametric four-wave mixing has been developed. Seeded parametric four-wave mixing requires only a single laser as an additional phase matched seeder field is generated via parametric four-wave mixing of the pump beam in a high gain cell. The seeder field travels collinearly with the pump beam providing efficient nondegenerate four-wave mixing in a second medium. This simple arrangement facilitates the detection of complex molecular spectra by simply scanning the pump laser. Seeded parametric four-wave mixing is demonstrated in both a low pressure cell and an air/acetylene flame with detection of the two-photon C (2) Pi(upsilon'=0)<--X (2) Pi(upsilon =0) spectrum of nitric oxide. From the cell data a detection limit of 10(12) molecules/cm(3) is established. A theoretical model of seeded parametric four-wave mixing is developed from existing parametric four-wave mixing theory. The addition of the seeder field significantly modifies the parametric four-wave mixing behaviour such that in the small signal regime, the signal intensity can readily be made to scale as the cube of the laser pump power while the density dependence follows a more familiar square law dependence, In general, we find excellent agreement between theory and experiment. Limitations to the process result from an ac Stark shift of the two-photon resonance in the high pressure seeder cell caused by the generation of a strong seeder field, as well as a reduction in phase matching efficiency due to the presence of certain buffer species. Various optimizations are suggested which should overcome these limitations, providing even greater detection sensitivity. (C) 1998 American Institute of Physics, [S0021-9606(98)01014-9].

Infrared seeded parametric four-wave mixing for sensitive detection of molecules

We have developed a sensitive resonant four-wave mixing technique based on two-photon parametric four-wave mixing with the addition of a phase matched ''seeder'' field. Generation of the seeder field via the same four-wave mixing process in a high pressure cell enables automatic phase matching to be achieved in a low pressure sample cell. This arrangement facilitates sensitive detection of complex molecular spectra by simply tuning the pump laser. We demonstrate the technique with the detection of nitric oxide down to concentrations more than 4 orders of magnitude below the capability of parametric four-wave mixing alone, with an estimated detection threshold of 10(12) molecules/cm(3).

Theoretical Analysis of Multimodal Four-Wave Mixing in Optical Microwires

Optical fiber microwires (OFMs) are nonlinear optical waveguides that support several spatial modes. The multimodal generalized nonlinear Schrodinger equation (MM-GNLSE) is deduced taking into account the linear and nonlinear modal coupling. A detailed theoretical description of four-wave mixing (FWM) considering the modal coupling is developed. Both, the intramode and the intermode phase-matching conditions is calculated for an optical microwire in a strong guiding regime. Finally, the FWM dynamics is studied and the amplitude evolution of the pump beams, the signal and the idler are analyzed.

Simulação do comportamento espectral de redes de período longo em fibra óptica

Esta tese é dedicada às redes de período longo, LPG’s, em fibra óptica, escritas por exposição a radiação ultravioleta (UV) ou por exposição a descargas eléctricas, e às suas aplicações em comunicações ópticas e em sistemas sensores. Numa primeira fase estudaram-se os aspectos teóricos fundamentais para a compreensão das LPG, nomeadamente os dois modelos matemáticos propostos na literatura, para a transmissão espectral de uma LPG, o modelo de duas camadas e o modelo de três camadas. Em seguida, estudou-se o deslocamento do comprimento de onda ressonante perante mudanças de parâmetros externos. Aqui, verificou-se que para variações da temperatura no exterior da LPG, o deslocamento do comprimento de onda ressonante é linear. Por outro lado, para variações de índice de refracção exterior, verificou-se que à medida que o índice exterior se aproxima dos valores do índice de refracção da bainha, o comprimento de onda ressonante tende para valores mais baixos. Por último, realizou-se um estudo da transmissão espectral de duas aplicações que envolvem LPG’s, nomeadamente dois tipos de interferómetros e filtros ópticos. Numa segunda fase, foi desenvolvida uma ferramenta de simulação destes modelos, que permitia não só a obtenção dos espectros de transmissão das LPG’s mas também a obtenção das curvas de phase matching em função do período da rede e do comprimento de onda ressonante. A aplicação permitia também a obtenção das curvas do deslocamento do comprimento de onda ressonante, perante variações do índice de refracção exterior ou da temperatura. Para além disso, essa ferramenta realiza a simulação dos espectros de transmissão de filtros ópticos e de interferómetros de Michelson e de Mach-Zehnder construídos com base em LPG’s. A última fase do trabalho, a componente laboratorial, foi realizada na Unidade de Optoelectrónica e Sistemas Electrónicos do INESC Porto, onde foram construídos e testados os dispositivos estudados anteriormente, com o intuito de validar a aplicação desenvolvida. A ferramenta de simulação demonstrou ser capaz de simular de forma adequada os diversos aspectos do comportamento das LPG’s que foram estudados. A comparação dos resultados obtidos permitiu concluir que o modelo mais correcto para o estudo das LPG’s é o modelo de três camadas, o que está de acordo com o esperado.

Frequency tunable continuous THz wave generation in a periodically poled fiber

An all-fiber approach to terahertz generation using a periodically poled optical fiber is proposed and experimentally demonstrated. In the proposed approach, a continuous-wave THz wave is generated at a periodically poled fiber by beating two optical wavelengths from two laser sources with the wavelength spacing corresponding to the frequency of the THz wave. The key component in the system is the periodically poled fiber, which is made by a twin-hole fiber with the fiber core residing between two holes. The twin-hole fiber is then thermally poled at a temperature of similar to 260 degrees C with a voltage of 3.3 kV applied to the silver electrodes inside the two holes to introduce second-order nonlinearity. The quasi phase matching (QPM) condition is achieved by periodically erasing the thermal poling induced second-order nonlinearity with an ultraviolet laser, which enhances the energy conversion efficiency. The proposed approach is validated by an experiment. The emission of a THz wave centered at 3.8 THz with an output power of 0.5 mu W is observed. The frequency tunability between 2.2 and 3.8 THz is also experimentally demonstrated.

Eine kontinuierliche Lyman-alpha-Quelle basierend auf Festkörperlasersystemen

In dieser Arbeit wird eine schmalbandige kontinuierliche kohärente Lyman-α-Quelle basierend auf Festkörperlasersystemen zur zukünftigen Kühlung von Antiwasserstoff vorgestellt. Die fundamentalen Festkörperlasersysteme ermöglichen es im Vier-Wellen-Misch-Prozess zur Erzeugung der Lyman-α-Strahlung nicht nur die 6^1S – 7^1S-Zwei-Photonen-Resonanz des Quecksilbers sondern erstmals auch die 6^1S – 6^3P-Ein-Photonen-Resonanz zur Erhöhung der Konversionseffizienz optimal zu nutzen. In ersten Messungen wurden 0,063nW Leistung bei Lyman-α erzeugt. Mit dieser Lyman-α-Quelle war es, durch die Nähe des ersten fundamentalen Lasers zur Ein-Photonen-Resonanz, erstmals möglich den kompletten Verlauf der Phasenanpassungskurve des Vier-Wellen- Misch-Prozesses aufzunehmen. Neben den fundamentalen Lasersystemen und der Lyman-alpha-Erzeugung selbst, wird in dieser Arbeit die Detektion der produzierten Lyman-α-Strahlung mit einem Photomultiplier vorgestellt, die soweit optimiert wurde, dass eine zuverlässige Abschätzung der erzeugten Leistung möglich ist. Für diesen Zweck wurde zudem ein Teststand aufgebaut, mit dem die Transmissivität der Optiken, welche in der Lyman-α-Apparatur verwendet werden, bei 121,56nm gemessen wurde. Des Weiteren wird hier eine vielseitige Rechnung vorgestellt, mit der die erzeugte Leistung bei Lyman-α, unter anderem in Abhängigkeit von der Temperatur, der Absorption des ersten fundamentalen Laserstrahls, dem Dichteprofil des Quecksilberdampfes und unter dem Einfluss eines Puffergases, bestimmt wird.

Einfluss der 6 1 S - 6 3 P-Resonanz auf die Lyman-alpha-Erzeugung in Quecksilber

In dieser Arbeit wird eine kontinuierliche, kohärente Strahlungsquelle bei 121,56nm, der Lyman-alpha Linie in Wasserstoff, vorgestellt. Diese Lyman-alpha Quelle soll zur zukünftigen Laserkühlung von Antiwasserstoff dienen. Die Strahlung wird durch Vier-Wellen-Mischen in Quecksilberdampf produziert. Dabei wird ein Festkörperlasersystem zur Erzeugung der Fundamentalstrahlen eingesetzt. Zur Erhöhung der nichtlinearen Suszeptibilität wird die 6^1S-7^1S Zwei-Photonen-Resonanz ausgenutzt. Zusätzlich wird mit Hilfe eines durchstimmbaren ultravioletten Lasersystems die 6^1S-6^3P Ein-Photon-Resonanz genutzt, was es erlaubt, die nichtlineare Suszeptibilität des Mischprozesses um Größenordnungen zu erhöhen. Um den Einfluss der 6^1S-6^3P Ein-Photon-Resonanz zu untersuchen, wurden zunächst die Phasenanpassungstemperaturen bei verschiedenen Verstimmungen der ultravioletten Strahlung zur 6^3P Resonanz vermessen und festgestellt, dass kleinere Verstimmungen zu niedrigeren Phasenanpassungstemperaturen führen. Es konnte sowohl theoretisch wie auch experimentell gezeigt werden, dass diese niedrigeren Phasenanpassungstemperaturen bei kleinen Verstimmungen der Erhöhung der Lyman-alpha Erzeugung durch die größere nichtlineare Suszeptibilität bei kleinen Verstimmungen entgegenwirken. Bei immer kleineren Verstimmungen zur 6^3P Resonanz limitiert die Absorption der ultravioletten Strahlung die Lyman-alpha Erzeugung. Ein positiver Effekt der niedrigeren Phasenanpassungstemperaturen ist, dass es möglich wird, auf das bisher nötige Puffergas in der Quecksilber-Dampfzelle zu verzichten, was die Lyman-alpha Erzeugung um einen Faktor 1,7 erhöht. Damit war es möglich, die bisherige Effizienz der Lyman-alpha Erzeugung zu verbessern. Es wurde eine Lyman-alpha Leistung von 0,3nW erreicht. Zusätzlich zum Einfluss der 6^3P Resonanz auf die Lyman-alpha Erzeugung wurde ein weiterer Effekt beobachtet. Durch die Nähe der 6^1S-6^3P Ein-Photon-Resonanz wird auch mehr Besetzung in das obere 7^1S Niveau der Zwei-Photonen-Resonanz gepumpt. Dadurch konnte erstmals eine kontinuierliche Lasertätigkeit auf der 6^1P-7^1S Linie in Quecksilber bei 1014nm beobachtet werden.

Ottimizzazione di un controllo di temperatura per diodi laser

In questo lavoro di tesi si studia un processo sperimentale necessario alla realizza- zione di un esperimento di Fisica Atomica. L’attivit`a svolta consiste nell’ottimizzazione dei paramentri di un algoritmo di con- trollo PI (proporzionale-integrale) atto a stabilizzare la temperatura di un Diodo Laser entro 1mK. Nella branca dell’Ottica Non Lineare (dove la polarizzazione del mezzo ha una rispo- sta non lineare al campo elettrico) si possono presentare casi in cui la birifrangenza del mezzo ha una forte dipendenza dalla temperatura. Questa pu o ` essere control- lata per il raggiungimento delle condizioni di phase matching. Le fluttuazioni di temperatura possono minare tramite la dilatazione termica la precisione di una ca- vit`a Fabry-Perot, utilizzata per controllare e misurare la lunghezza d’onda della luce, dato che nominalmente ∆ν/ν = − ∆L/L. Negli esperimenti di Laser Cooling infi- ne si lavora spesso con transizioni la cui larghezza naturale Γ ∼ 1MHz , mentre la frequenza di un laser pu o ́ dipendere dalla temperatura con coefficienti tipicamente dell’ordine del GHz/K. Questa stabilizzazione risulta dunque fondamentale per una vasta classe di esperi- menti nei quali le derive termiche possono influenzare drammaticamente il processo di misura. La tesi, in particolare, si apre con un capitolo nel quale si tratta brevemente il con- testo matematico di riferimento per i sistemi di controllo a retroazione. Tra questi e ` di particolare interesse la regolazione proporzionale-integrale. Il secondo capitolo si concentra sulla caratterizzazione del sistema in oggetto al fine di trovare la sua funzione di trasferimento ad anello aperto. Nel terzo capitolo infine, si utilizzano gli strumenti matematici descritti precedente- mente per ottimizzare i parametri del regolatore e si discutono i risultati ottenuti e le misure finali.

Supersymmetric Mode Converters

Originally developed in the context of quantum field theory, the concept of supersymmetry can be used to systematically design a new class of optical structures. In this work, we demonstrate how key features arising from optical supersymmetry can be exploited to control the flow of light for mode division multiplexing applications. Superpartner configurations are experimentally realized in coupled optical networks, and the corresponding light dynamics in such systems are directly observed. We show that supersymmetry can be judiciously utilized to remove the fundamental mode of a multimode optical structure, while establishing global phase matching conditions for the remaining set of modes. Along these lines, supersymmetry may serve as a promising platform for versatile optical components with desirable properties and functionalities.

Nondiffracting Bessel plasmons

We report on the existence of nondiffracting Bessel surface plasmon polaritons (SPPs), advancing at either superluminal or subluminal phase velocities. These wave fields feature deep subwavelength FWHM, but are supported by high-order homogeneous SPPs of a metal/dielectric (MD) superlattice. The beam axis can be relocated to any MD interface, by interfering multiple converging SPPs with controlled phase matching. Dissipative effects in metals lead to a diffraction-free regime that is limited by the energy attenuation length. However, the ultra-localization of the diffracted wave field might still be maintained by more than one order of magnitude.