TL;DR: In this paper, a femtosecond adiabatic compression of femto-cond pulse can be achieved by employing the management of quadratic cascading nonlinearity in quasi-phase-matching gratings.
Abstract: We experimentally demonstrate that adiabatic compression of femtosecond pulse can be achieved by employing the
management of quadratic cascading nonlinearity in quasi-phase-matching gratings. Cascading nonlinearity is not a
simple analogy with third-order optical nonlinearity in term of the engineering properties of the magnitude and focusing
(or defocusing) nonlinearity. Femtosecond pulse compression is investigated based on type-I (e: o + o) collinear QPM
geometry of aperiodically poled MgO-doped LiNbO 3 (MgO: LN). Group-velocity-matching condition is chosen to
generate quadratic femtosecond soliton consisting of fundamental (FF) and second harmonic (SH) pulses. Adiabatic-like
compression process is observed in the length of 50 mm linearly chirped QPM. Cascading nonlinearity is local managed,
instead of dispersion management used in fiber adiabatic soliton compression. Quadratic soliton including FF and SH
pulses are obtained from the compression of 95 fs FF pulse in the initial experiments. Dependence on the phase
mismatch and group velocity mismatch, cascading nonlinearity has a flexible property and presents a new challenge for
exploring femtosecond pulse shaping and control. The demonstrated pulse compression and control based on cascading
nonlinearity is useful for generation of shorter pulses with clean temporal profiles, efficient femtosecond second
harmonic generation and group-velocity control.
TL;DR: In this paper, the authors demonstrated how white light was generated when the ultrashort pulse propagated in a tapered fiber with anonymous dispersion, showing that the Stimulated Raman Scattering effect plays an important role in the long wave range of the supercontinuum.
Abstract: Dispersion property is an important fact to generate white light. Different structures could change the dispersion
properties of fibers. This paper demonstrates how the white light was generated when the ultrashort pulse propagated in a
tapered fiber. We simulated how the supercontinuum was generated in a variety of tapered fibers which have different
parameters. The supercontinuum range could be reached from 680nm to1750nm. It is shown that the width and the shape
of the supercontinuum depend on both the fiber parameters such as the diameter or the length of tapered waist regime
and pulse peak power. The paper also discussed the influence of the different dispersion and nonlinear effects in detailed,
including GVD (Grouped Velocity Dispersion), SPM (Self Phase Modulation), TOD (Third Order Dispersion), SS (Self
Steeping), and SRS (Stimulated Raman Scattering). Through the numerical simulation, it presents when the ultrashort
pulse propagates in tapered fibers with anonymous dispersion, the Stimulated Raman Scattering effect plays an important
role in the long wave range of the supercontinuum. The influence of the higher order dispersion, especially third order
dispersion, on the anti-Stokes part in the supercontinuum process was also discussed. A smoother and broader
supercontinuum could be obtained after choosing the suitable parameters of the tapered optical fibers, especially the
diameter or the length of tapered waist regime.
TL;DR: In this article, the influence of the chromatic dispersion and the nonlinearity in fiber on chaotic synchronization has been investigated based on the theoretical models used to describe the dynamics of semiconductor laser subjected to the external optical feedback and signal transmission in fiber channel.
Abstract: In order to supply a theoretical guide for chaotic telecommunication, the influences of the chromatic dispersion and
nonlinearity in fiber on the chaotic synchronization have been investigated based on the theoretical models used to
describe the dynamics of semiconductor laser subjected to the external optical feedback and signal transmission in fiber
channel. The numerical simulation results show that, the fiber nonlinear effect is responsible for the phase varying of
chaotic signal and do not affect the amplitude of the chaotic signal; due to chromatic dispersion, the amplitude
characteristics of chaotic signal are distorted significantly and the system synchronization quality will be impaired; after
propagating 200km in dispersion shifted fiber, a desirable system chaotic synchronization with a synchronized
coefficient 0.99 can be achieved by adopting a amplifier before the received laser to compensate the fiber loss.
TL;DR: In this article, the nonlinear optical properties of perylene derivatives were studied by femtosecond Z-scan technique using femto-conditional laser for 2-photon absorption cross-sections.
Abstract: Nonlinear optical properties of perylene derivatives were studied by femtosecond Z-scan technique. 3,4,9,10-Perylenetetracarboxylic dianhydride (PTCDA), 3,4,9,10-perylenetetracarboxylic diimide (PTCDI), and perylene-66
(dibenzthiophenoperylene-N,N'-dicyclohexylimide), were studied. Tetrahydrofuran was used as a solvent for perylene-
66. The solubility of PTCDA and PTCDI is very poor. Their colloidal solution was prepared by the irradiation of the
third harmonics of a pulsed YAG laser to opaque suspension of PTCDA and PTCDI. Transparent colloidal solution was
obtained within 50 minutes of UV irradiation. Colloidal solution of quinacridone was also studied. Two-photon
absorption cross sections of these dyes were measured by open aperture Z-scan method using a femtosecond laser. The
dependence of two-photon cross section on laser wavelength was measured in the wavelength range of 780-820 nm.
TL;DR: In this paper, the authors proposed a double-pass DC-OFS with double pass configuration for the first time, where the available nonlinear crystal length is used twice: forward for SFG and backward for DFG in each conversion and this device is called double pass SFG+DFG wavelength converter.
Abstract: In this paper, we proposed a novel variable operation of a DC-OFS based on double SFG+DFG nonlinearity process
with double-pass configuration for the first time. In this scheme, the available nonlinear crystal length is used twice:
forward for SFG and backward for DFG in each conversion and this device is called double-pass SFG+DFG wavelength
converter as the SF wave propagates twice in the waveguide. We used the novel multiple-quasi-phase-matched LiNbO 3
(M-QPM-LN) waveguides having the continuously-phase-modulated domain structure, which can be operated by
multiple pump wavelengths with minimum loss of efficiency. The frequency spacing of control signal-a is twice as large
as the control signal-b. Conversion bandwidth is the frequency difference of control signal-b and control signal-a. We
discussed Double-SFG+DFG-OFS with double-pass configuration theoretically and gave the formula of the input power
of input signal, the two controlling light and pump light, which proposed a simple and feasible way to optimize the
performance of the device. In this scheme, the advantages of the cascaded SFG+DFG scheme and the DC-OFS scheme
are combined to a great extent. We believe this double-pass cascaded SFG+DFG DC-OFS must be better than single-pass
cascaded SFG+DFG DC-OFS for constructing future flexible photonic networks.
TL;DR: In this paper, a femtosecond (fs) laser pulses around 800 nm were used to generate photoluminescence in ZnO material under detuning condition.
Abstract: Multi-photon excitation in ZnO material by femtosecond (fs) laser pulses around 800 nm was clearly observed.
Under the intense field generated by fs pulses, two-photon absorption process was found very efficient in the
excitation of the band edge emission from ZnO material under detuning condition. Nonlinear optical effects, such as
Stark effect and Rabi effect, that may emerge under intense field are suggested to be responsible for this efficient
excitation via two-photon absorption process. We consider that this NLO route to generate photoluminescence in
ZnO material is meaningful in the research of blue-violet semiconductor laser field.
TL;DR: In this article, the authors investigated sol-gel-processed TiO 2 /SiO 2 films doped with organic azo dye and found that the nonlinearity is stable at 80°C for at least 2 hours and 120°C at least 1 hour.
Abstract: Sol-gel-processed TiO 2 /SiO 2 films doped with organic azo dye have been investigated. The film was spin-coated on the
ITO coated glass substrate and rapidly condensed by evaporation of the solvent from the liquid film. The thickness of the
hybrid films can be varied from 0.2 to 0.6 micron. When the prehydrolyzed tetraethoxysilane (TEOS) sol and titania
precursor(titanium butoxide) are mixed together with various molar ratios, the refractive index of the film may vary from
1.49 to 1.81 at 1300nm. The film is aged at 80°C for 2 h and then corona poled at 120°C for 1 h so that the dye molecules
are dispersed in numerous pores of the oxide matrix. The absorbance spectra of the film measured by a UV-visible
spectrophotometer show that the process of aging and poling in the sample preparation causes the pores in the oxide
matrix to shrink and nonlinear molecules are aligned in the direction of the poling field and are trapped in the pores. The
electro-optic coefficient r 33 is 42 pm/V at a fundamental wavelength of 1300nm. The nonlinearity is stable at 80°C for
2500h at least. The excellent thermal stability of the hybrid organic/inorganic film is an advantage for optical
applications.
TL;DR: In this paper, a series of symmetrically substituted phenylenevinylene chromophores with different lengths of conjugated chains and different electro negativity of substitution groups were used to provide an insight into the nature of the two-photon absorption (TPA) processes and reveal structure-property relations.
TL;DR: In this article, a copolarization dual-pump configuration in a highly nonlinear photonic crystal fiber (PCF) with two fiber Bragg connections and a Faraday rotator mirror is demonstrated.
Abstract: A basic scheme of the polarization insensitive four-wave-mixing all-optical wavelength conversion with a copolarization
dual-pump configuration in a highly nonlinear photonic crystal fiber (PCF) is demonstrated. With two fiber Bragg
Gratings and a Faraday rotator mirror, both the pumps and the signal make a dual pass through a highly nonlinear PCF.
The rotation of the signal polarization by the Faraday rotator mirror guarantees that both orthogonal polarization
components of the signal will efficiently mix with the two pumps to produce a polarization-insensitive multi-wavelength
conversion. The design and simulation of the bismuth oxide-based PCF indicate that the desired dispersion properties can
be tailored by the geometrical parameters of PCF microstructure. The propagation loss at 1550nm is about 0.8dB/m. The
nonlinear coefficient is expected to be 1100W -1 km -1 by using bismuth oxide-based glass and reducing the effective core
area. The mode-field diameter of PCF is estimated to be 1.98μm and the predicted effective core area is 3.3μm 2 . The
polarization insensitive four-wave-mixing wavelength converter with copolarization dual-pump configuration shows the
small polarization sensitivity, the high conversion efficiency and the simultaneous multi-wavelength conversion.
TL;DR: A novel numerical algorithm for nth-order cascaded Raman fiber lasers with the combination of genetic algorithm (GA) and shooting method which can effectively and quickly solve the coupled equations of the CRFL without the problem of divergence.
Abstract: In this paper, we proposed a novel numerical algorithm for nth-order cascaded Raman fiber lasers (CRFLs) with the
combination of genetic algorithm (GA) and shooting method. Although shooting method possesses fast speed in solving
nonlinear two-point boundary-value ordinary differential equations, calculating process may diverge if it is directly
applied in the coupled equations of CRFLs when arbitrarily guessed initial values are out of the domain of convergence.
To overcome the problem, genetic algorithm which has rather strong searching ability in global space is firstly employed
to search for the initial value in convergent domain for each Stokes power; and then, the task of finding the more
accurate initial values is finished by shooting method instead of GA whose searching ability is weak in local region. As
an example, a sixth-order Ge-doped CRFL has been simulated by the novel algorithm. Calculated results show that the
new method can effectively and quickly solve the coupled equations of the CRFL without the problem of divergence.
TL;DR: In this article, the effect of the order of soliton on the evolution of signal pulse and the changing of root mean square width of signal was investigated by solving three nonlinear Schrodinger equations numerically.
Abstract: The ultra-short pulse optical parametric amplification based on continuous wave pump and pulse signal model is
investigated by solving three nonlinear Schrodinger equations numerically. The effect of the order of soliton is presented
by comparing the evolution process of signal pulse and the changing of root mean square width of signal. The
phenomenon of signal pulse splitting and the broadening of the pulse will appear in the amplification process. Larger
order of the soliton makes the pulse split at first, then begin to broaden. Smaller order of the soliton leads to the
broadening of pulse firstly, then the pulse begin to split after propagating in a section of fiber.
TL;DR: In this article, the nonlinear dynamic characteristics of an optical injection VCSEL are investigated numerically, and the simulated results show that VCSels can exhibit periodic oscillations, deterministic chaos and other complex instabilities under optical injection.
Abstract: In this paper, after taking into account two situations that the polarization of the injection light is parallel or orthogonal
with the solitary vertical-cavity surface-emitting laser (VCSEL) output light, the nonlinear dynamic characteristics of an
optical injection VCSEL are investigated numerically. The simulated results show that VCSEL can exhibit periodic
oscillations, deterministic chaos and other complex instabilities under optical injection. For parallel or orthogonal optical
injection, the same injection coefficients have different effects on the output of VCSEL. By properly adjusting the
injection strength or detuning frequency, the dynamical state of the laser output can be controlled to a fixed state, and the
polarization of the VCSEL output light can also be controlled.
TL;DR: In this paper, all-optical frequency up-conversions of an optical IF signal to the upper frequency band using FWM without serious crosstalk is theoretically analyzed, and main factors related to the conversion efficiency are presented.
Abstract: In this paper, all-optical wavelength conversion based on FWM in ROF system is theoretically analyzed. It can be used
to generate the optical millimeter wave signals and to implement the all-optical frequency up/down conversion in ROF
systems. Due to the ultrafast nonlinear response of the HNL-DSF, it is possible to realize terahertz waveform all-optical
mixing or up-conversion. All-optical frequency up-conversions of an optical IF signal to the upper frequency band using
FWM without serious crosstalk were demonstrated. Based on analysis of the all-optical wavelength conversion in high-nonlinear
fiber, main factors related to the conversion efficiency are presented. Methods to increase the conversion
efficiency have been discussed. With the longer high-nonlinear fiber, the higher nonlinear coefficient, the appropriate
power of the pump, the appropriate polarization between the signal and the bump, and high efficiency to implement the
wavelength conversion can be achieved. The theoretical analysis is verified by the simulation results.
TL;DR: Simulation results show that SOA XGM sampler can efficiently sample low repetition rate optical short pulse or short pulse with poor stability and sampling error caused by ASE noise of SOA, thermal noise of PIN and time-domain jitter of control pulse is discussed.
Abstract: A simple and low-cost all-optical equivalent-time sampling system is present. The optical sampling was realized by XGM in SOA and pulse-broadening in low-bandwidth PIN. A system model is funded based on noisy SOA dynamic function and a simplified equivalent electric circuit model about PIN. The sampling-recovery process had been simulated to validate the measuring capability of the sampler. Sampling error caused by ASE noise of SOA, thermal noise of PIN and time-domain jitter of control pulse is discussed too. Simulation results show that SOA XGM sampler can efficiently sample low repetition rate optical short pulse or short pulse with poor stability.
TL;DR: In this paper, a nonlinear fiber with carbon disulfide was designed by filling a highly nonlinear liquid into hollow-core photonic crystal fibers, which can be more than 20 times larger than that of a conventional PCF.
TL;DR: In this article, the authors investigated the nonlinear dynamics of a single cavitation bubble near an elastic boundary using optical beam deflection (OBD) and determined the maximum bubble radii and the bubble life time for each oscillation cycle according to the characteristic signals.
Abstract: Nonlinear dynamics of a laser-generated single cavitation bubble near an elastic boundary is investigated by a fiber-optic
diagnostic technique based on optical beam deflection (OBD). The maximum bubble radii and the bubble life-time
for each oscillation cycle are determined according to the characteristic signals. It is shown that with the increase of the
number of oscillating cycles, the maximum radii and the life-time of the bubble are decreased sharply. Furthermore, the
effect of material elasticity on nonlinear dynamics of cavitation bubble has also been investigated in some detail. The
maximum bubble size and thus the bubble life time decreases with an increase in elastic modulus. In addition,
increasing elastic modulus leads to a significant decrease of the collapse amplitude and the bubble energy. These results
are valuable in the fields of cavitation erosion, collateral damage in laser surgery, and cavitation-mediated enhancement
of pulsed laser ablation of tissue.
TL;DR: In this paper, a ring cavity is side-coupled to one arm and a phase shifter is introduced into the other arm for static phase compensation to tune the system between zero and complete transmission, with a phase offset much narrower than the full width of the cavity resonance itself.
Abstract: A novel configuration of ring cavity-coupled Michelson interferometer is proposed to create sharp asymmetric multiple-resonance
line shape, in which a ring cavity is side-coupled to one arm and a phase shifter is introduced into the other
arm for static phase compensation. Such asymmetric line shape allows the tuning of the system between zero and
complete transmission, with a phase offset much narrower than the full width of the cavity resonance itself. As tuning
between resonance peak and notch of such asymmetric profile, optical transmission becomes much more sensitive to the
round-trip phase shift of ring cavity than that in the case of symmetric Lorentzian line shape. By cooperating Kerr
nonlinearity and cavity feedback, novel hysteresis loops and intrinsic bistability are achievable by adjusting incident
power. The shapes of hysteresis curves associated with asymmetric resonance line shape are different from those arising
from symmetric line shape. By adjusting the static phase compensation of phase shifter, tunable hysteresis loop and
asymmetric multiple-resonance transmission can be easy performed. The simply constructed device is a good reference
for sensitive optical switch, filter and sensor.
TL;DR: In this paper, the phase conjugation properties of self-pumped and mutually pumped phases were investigated in a Cu:KNSBN crystal with Q-switched single longitudinal mode and pulse laser pumping.
Abstract: The phase conjugation properties of self-pumped phase conjugation (SPPC), mutually pumped phase conjugation
(MPPC), SPPC and MPPC coexisting are researched in Cu:KNSBN crystal with Q-switched single longitudinal mode
YAG pulse laser pumping. The dependence of the reflectivity of phase conjugation on the incidence position and angle
are obtained experimentally. The results show the optimal incident parameter exists in photorefractive phase
conjugation effect.
TL;DR: In this paper, the formation and propagation of dark electromagnetic solitons in metamaterials was studied, and the authors used an extended Tanh-function expansion method to solve the nonlinear equation for ultrashort electromagnetic pulse propagation with a nonlinear polarization.
Abstract: Solitons have been found in many physical branches. Previous investigations on solitons mainly focused on various
nonlinear dispersive media in nature. It is well known that in the nonlinear dispersive medium, soliton formation is due
to the exact balance between the nonlinearity and the group velocity dispersion (GVD). When the signs of nonlinearity
and GVD are the same, that is, the positive (focusing) nonlinearity vs. positive (normal) GVD, or the negative
(defocusing) nonlinearity vs. negative (anomalous) GVD, the interaction between nonlinearity and GVD may lead to the
generation of dark solitons. In this paper, we study the formation and propagation of dark electromagnetic solitons in the
metamaterials, artificial structures that display properties beyond those available in naturally occurring materials. We use
an extended Tanh-function expansion method to solve the nonlinear equation for ultrashort electromagnetic pulse
propagation in metamaterial with a nonlinear polarization, and get dark solitary solutions under various conditions. It is
found that, due to the role of the second-order nonlinear dispersion resulted from the dispersive magnetic permeability,
dark solitons can be formed in the absence of linear dispersion, or even in the case of anomalous linear GVD for a
focusing nonlinearity, challenging the traditional conditions for dark soliton formation.
TL;DR: In this article, the authors extended occurrences of bistable chromatic switching to a new rare-earth-doped system, namely single Tmdoped laser crystal pumped at 648 nm avalanche wavelength.
TL;DR: The first-order hyperpolarizabilities of H-shape azobenzenes in gas and in THF have been theoretically studied by Hartree-Fock method and basis set sto-3g with Onsager model as mentioned in this paper.
Abstract: First-order hyperpolarizabilities of H-shape azobenzenes in gas and in THF have been theoretically studied by Hartree-Fock method and basis set sto-3g with Onsager model, including 4,5-bis((E)-(4-nitrophenyl)diazenyl)anthracene-1,8-diol, 4,5-bis((E)-(4-(trifluoromethyl)phenyl)diazenyl)anthracene-1,8-diol, 4,5-bis((E)-(3-chloro-4-fluorophenyl)diazenyl)
anthracene-1,8-diol and 4,5-bis((E)-(4-chlorophenyl)diazenyl)anthracene-1,8-diol. Compared with corresponding
azobenzene monomers, H-shape azobenzenes had much larger first-order hyperpolarizabilities. There were four factors
which could obviously influence their first-order hyperpolarizabilities. Firstly, H-shape azobenzenes possessed dihedral
angles of approximate ten degrees caused by coulomb repulsions with weakening dipole's changes between ground
states and excited states. Meanwhile, dihedral angle induced energy gap between HOMO and LUMO to increase.
Secondly, dipole-dipole interaction was considered as perturbation which caused strong energy splitting of each
molecular orbital with the lessening of energy gap. Thirdly, hyper-conjugated effect existed in H-shape azobenzene and
it induced energy gap to decline. Fourthly, solvent effects could obviously enhance their first-order hyperpolarizabilities
by comparing results in gas with results in THF. These factors competed and affected each other. The latter three factors
lastly overcame coulomb repulsion, which explained that H-shape azobenzenes' first-order hyperpolarizabilities were
much larger than corresponding monomers'.
TL;DR: In this article, the dispersion relation of a dimensional periodic structure is analyzed and slow Bragg soliton solutions are given by assuming adiabatic evolution of the soliton passed through fiber Bragg grating which is apodized by using a hyperbolic tangent apodization function in the middle of the FBG.
Abstract: On the basis of non-linear coupled-mode theory, the dispersion relation of a dimensional periodic structure is analyzed and slow Bragg soliton solutions are given. The approximation approach for non-linear coupled-mode theory is studied by assuming adiabatic evolution of the soliton passed through fiber Bragg grating which is apodized by using a hyperbolic tangent apodization function in the middle of the FBG. And in the presence of apodization, the velocity equation of Bragg soliton is found. In this paper, we have simulated the motion tracks and velocities of Bragg solitons, analyzed effects of different parameters on motion track and velocity of Bragg soliton, and obtained different timedisplacement curves and time-velocity curves. It is shown that the final steady velocity of soliton can be found by choosing specifical parameters, thereby, slow Bragg solitons whose propagate velocity through the grating is far lower than the speed of light in glass can obtained. We have presented detailed simulative results that agree with theoretical analysis.
TL;DR: In this paper, the three-photon absorption (3PA) properties of nonlinear organic materials were studied using a femtosecond Ti:sapphire oscillator-amplifier laser system associated with an optical-parametric amplifier.
Abstract: We have demonstrated efficient three-photon excitation in a number of nonlinear organic materials developed
at our center or in cooperation with other research groups. The three-photon absorption (3PA) properties of
these materials are studied using a femtosecond Ti:sapphire oscillator-amplifier laser system associated with an
optical-parametric amplifier. Considering the transverse intensity distribution of the incident beam during
measurements, the 3PA induced nonlinear transmission of the incident beam with a Gaussian transverse spatial
profile is derived. Some of the 3PA-active materials are highly fluorescent while some others are
nonfluorescent. In one of these materials, vibrational resonance enhanced broadband multiphoton absorption
was founded. These materials can be used in optical power limiting and stabilization, frequency-upconversion
imaging and microscopy etc. Some recent experiments of three-photon pumped power limiting and stabilization
are briefly presented.
TL;DR: In this article, a bilayer consisting of a subwavelength layer of linear negative index material (NIM) and a Kerr-type nonlinear layer of conventional positive index material was considered as a combined defect for a one-dimensional photonic crystal and investigated the effect of the thin film on the hysteretic behavior of the Goos-HA¤nchen shift and the incident intensity.
TL;DR: In this paper, femtosecond degenerate four-wave mixing (DFWM) was used to measure the third-order optical nonlinearities of squarylium and croconium dyes in methanol solution.
TL;DR: In this article, the authors used difference frequency generation (DFG) in AGS or AGSe crystals by pumping with the output of an optical parametric oscillator to achieve mid-infrared radiation.
TL;DR: In this article, a novel optical coding method for all-optical analog-to-digital conversion using nonlinear optical switches based on the Sagnac interferometer is proposed, which can overcome the obstacles of inherently limited operating speed of electronic ADC.
Abstract: Self- and cross-phase modulation (SPM, XPM) in fiber is expected to play a major role in ultrafast all-optical analog-to-digital conversion(ADC), which can overcome the obstacles of inherently limited operating speed of electronic ADC.
In this paper, we propose novel optical coding method for all-optical ADC using nonlinear optical switches based on the
Sagnac interferometer. The multiperiod transfer function, which is the key to coding, is achieved through an exact design
of the Sagnac interferometer. We conducted proof-of-principle experiments and successfully demonstrated 2.6-bit all
optical ADC with Gray code output. The proposed optical coding, combined with existing optical sampling and
quantizing techniques, will enable ultrafast photonic ADC without electronics.
TL;DR: In this paper, the effect of local environment on small molecules of Disperse Red 1 and their dynamic behavior is studied, and it is shown that dye-polymer interaction can be the dominant factor in local environment around the dye molecules.
Abstract: In order to improve the efficiency of optical polymers' function in photonic applications, the effect of local
environment on small molecules of Disperse Red 1 and their dynamic behavior is studied. Poly Styrene Sulfonic Acid
polymer used as host material to make highly doped polymeric thin films. By studying the samples' spectra in vitro and
in situ, and investigating the photo-anisotropic effects on samples, it is shown that dye-polymer interaction can be the
dominant factor in local environment around the dye molecules. Therefore, it can be used to increase significantly the
response intensity and improve the performance of photonic devices.
TL;DR: In this paper, the effect of lattice modulation on small-scale self-focusing of beam in optical lattice is studied both analytically and numerically, and it is investigated how the perturbation changes with lattice modifications.
Abstract: In this paper, we consider spatial soliton propagation in Kerr nonlinear media with harmonic modulation of the refractive
index, and investigate the effect of the lattice modulation for small-scale self-focusing of beam in optical lattice. Based
on the modulation instability theory, the effect of lattice modulation on small-scale self-focusing of beam in optical
lattice is studied both analytically and numerically. It is investigated how the perturbation changes with lattice
modulation. Comparing the gain spectrum in lattice modulation with that without lattice modulation, we find that without
the lattice modulation the perturbation gain increases with the input power when the input power is large enough to
initiate the modulation instability. The gain of the noise is controlled when the lattice modulation is induced.