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1.
Opt Lett ; 48(1): 121-122, 2023 Jan 01.
Article in English | MEDLINE | ID: mdl-36563378

ABSTRACT

A first, to the best of our knowledge, demonstration of passive mode-locking in diode-pumped alkali laser (DPAL) is reported in this paper. An intracavity cesium vapor cell, buffered by atmospheric pressure methane, is used to passively mode lock a continuously pumped cesium DPAL with a static gain medium. A train of short pulses with duration less than 460 ps was observed using a 2.0-GHz bandwidth detector that limited the real time duration measurements. The calculated minimum duration for these pulses is 57 ps.

2.
Opt Express ; 26(8): 9792-9797, 2018 Apr 16.
Article in English | MEDLINE | ID: mdl-29715925

ABSTRACT

We describe a method of line narrowing and frequency-locking a diode laser stack to an alkali atomic line for use as a pump module for Diode Pumped Alkali Lasers. The pump module consists of a 600 W antireflection coated diode laser stack configured to lase using an external cavity. The line narrowing and frequency locking is accomplished by introducing a narrowband polarization filter based on magneto-optical Faraday effect into the external cavity, which selectively transmits only the frequencies that are in resonance with the 62S1/2 → 62P3/2 transition of Cs atoms. The resulting pump module has demonstrated that a diode laser stack, which lases with a line width of 3 THz without narrowbanding, can be narrowed to 10 GHz. The line narrowed pump module produced 518 Watts that is 80% of the power generated by the original broadband diode laser stack.

3.
Opt Express ; 26(5): 5497-5500, 2018 Mar 05.
Article in English | MEDLINE | ID: mdl-29529752

ABSTRACT

We performed a measurement of the beam quality of an optimized moderate power cesium Diode Pumped Alkali Laser (DPAL). The DPAL used a stable resonator and operated in continuous wave mode using a static cell filled with metallic cesium and a mixture of methane and helium at 200 and 400 torr respectively. In this work, we characterized the spatial quality of the DPAL output beam. As a result of these experiments we determined the output beam quality was excellent (M2 < 1.2) in the whole range of pump power used (up to 11.5W) and pump intensities reaching 1.5 kW/cm2. The optical conversion efficiency of this laser was 51% and the slope efficiency was 61%.

4.
Opt Express ; 24(17): 19286-92, 2016 Aug 22.
Article in English | MEDLINE | ID: mdl-27557208

ABSTRACT

A Mach-Zehnder interferometer was used for contactless measurement of the temperature of the gain medium within a static cell of Cs DPAL. The maximum temperature recorded approached 700° C leading to a significant degradation of laser performance. This work also examined lasing and non-lasing heat deposition and has shown that as much as 85% of the heating in a DPAL gain medium can be attributed to quenching.

5.
Rev Sci Instrum ; 86(8): 083104, 2015 Aug.
Article in English | MEDLINE | ID: mdl-26329171

ABSTRACT

This paper presents results of cooperative efforts on development of a continuous wave Cs diode pumped alkali laser with moderate output power, which can be considered as a prototype of the commercial device. The developed system operates at 895 nm with output power about 4 W and slope efficiency 28%. Measured turn on time of this system from the standby mode is about a minute.

6.
Opt Lett ; 40(1): 119-22, 2015 Jan 01.
Article in English | MEDLINE | ID: mdl-25531624

ABSTRACT

The two-dimensional (2D) temperature profiles of an active-gain medium in a Cs + methane diode pumped alkali laser (DPAL) have been experimentally measured. This nonperturbative technique uses a Mach-Zehnder interferometer, which is longitudinally coupled into the cavity of an operating alkali laser to probe the distortion of the optical path length in the gain medium due to heating. The resulting interferograms are analyzed using the commercial program QuickFringe to quickly and accurately measure the distortion through which the temperature profile can be determined. For a 9 W Cs + methane DPAL being pumped with 20 W of resonant D2 light, a maximum temperature rise of 58°C is observed.

7.
Opt Lett ; 39(3): 528-31, 2014 Feb 01.
Article in English | MEDLINE | ID: mdl-24487857

ABSTRACT

Utilizing two-photon excitation in hot Rb vapor we demonstrate the generation of collimated optical fields at 420 and 1324 nm. Input laser beams at 780 and 776 nm enter a heated Rb vapor cell collinear and circularly polarized, driving Rb atoms to the 5D(5/2) state. Under phase-matching conditions coherence among the 5S(1/2)→5P(3/2)→5D(5/2)→6P(3/2) transitions produces a blue (420 nm) beam by four-wave mixing. We also observe a forward and backward propagating IR (1324 nm) beam, due to cascading decays through the 6S(1/2)→5(1/2) states. Power saturation of the generated beams is investigated by scaling the input powers to greater than 200 mW, resulting in a coherent blue beam of 9.1 mW power, almost an order of magnitude larger than previously achieved. We measure the dependences of both beams in relation to the Rb density, the frequency detuning between Rb ground-state hyperfine levels, and the input laser intensities.

8.
Theranostics ; 3(4): 282-8, 2013.
Article in English | MEDLINE | ID: mdl-23606915

ABSTRACT

We report a localized surface plasmon enhanced upconversion luminescence in Au/SiO2/Y2O3:Yb3+,Er3+ nanoparticles when excited at 980 nm. By adjusting the silica spacer's thickness, a maximum 9.59-fold enhancement of the green emission was obtained. Effect of the spacer distance on the Au-Y2O3:Yb3+, Er3+ green upconversion mechanism was numerically simulated and experimentally demonstrated. In theory for radiative decay and excitation rates, they can be largely enhanced at the spacer thicknesses of less than 70 and 75 nm, respectively, and the quenching can be caused by the non-radiative energy transferring at the distance of less than 55 nm.


Subject(s)
Gold/chemistry , Luminescence , Nanoparticles/chemistry
9.
Opt Lett ; 37(10): 1637-9, 2012 May 15.
Article in English | MEDLINE | ID: mdl-22627521

ABSTRACT

Employing ultrafast laser excitation and time-correlated single-photon counting, we have measured the fine-structure transfer between Rb 5P states induced by collisions with 4He buffer gas at temperatures up to 150 °C. The temperature dependence of the binary cross section agrees with earlier measurements. Our data show that the temperature dependence of the three-body rate is about the same as that of the binary rate. The three-body rate can be described as arising from the reduction of the rubidium fine-structure splitting due to nearby helium atoms.

10.
Opt Express ; 19(8): 7894-902, 2011 Apr 11.
Article in English | MEDLINE | ID: mdl-21503101

ABSTRACT

We have calculated photoionization rates in alkali lasers. The photoionization of alkali atoms in the gain medium of alkali lasers can significantly degrade the laser performance by reducing the neutral alkali density and with it the gain. For a ten atmosphere Rb laser and a Cs exciplex laser, the photoionization induced alkali atom loss rates are greater than 10(5) sec(-1). These high loss rates will quickly deplete the neutral alkali density, reducing gain, and may require fast, possibly, supersonic flow rates to sufficiently replenish the neutral medium for CW operation.

11.
Opt Express ; 18(15): 15553-9, 2010 Jul 19.
Article in English | MEDLINE | ID: mdl-20720935

ABSTRACT

Tunable extraordinary transmission via changing temperature of a porous metallic layer on top of a thin layer of dielectric strontium titanate (STO) was studied. The metallic layer has a through-hole array and each hole has a circular converging-diverging channel (CDC) shape, which induces the excitation of surface plasmon polaritons (SPPs) and then results in a controllable extraordinary optical transmission in the terahertz (THz) frequency range. We used a three-dimensional (3D) finite element method to analyze the transmission characteristics of the structure. Location and magnitude of the transmission peaks can be adjusted by hole size, converging angle, and thicknesses of metal and STO layers. Remarkably, the suggested structure presents a strong transmission dependency on temperature, which offers a new approach to actively and externally tune the transmission. This new design could lead to a family of temperature-sensitive devices working in the THz frequency range, promising in many applications including photonics, nanolithography, imaging, and sensing.

12.
Opt Lett ; 35(13): 2146-8, 2010 Jul 01.
Article in English | MEDLINE | ID: mdl-20596175

ABSTRACT

Using ultrafast laser excitation and time-correlated single-photon counting techniques, we have measured the collisional mixing rates between the rubidium 5(2)P fine-structure levels in the presence of (4)He gas. A nonlinear dependence of the mixing rate with (4)He density is observed. We find Rb fine-structure transfer is primarily due to binary collisions at (4)He densities of < or = 10(19) cm(-3), while at greater densities, three-body collisions become significant. We determine a three-body collisional transfer rate coefficient (5(2)P(3/2) --> 5(2)P(1/2)) of 1.25(9)x10(-32) cm(6)/s at 22 degrees C.

13.
Opt Express ; 18(5): 4428-33, 2010 Mar 01.
Article in English | MEDLINE | ID: mdl-20389455

ABSTRACT

We observe a novel type of vector dark soliton in a fiber ring laser. The vector dark soliton consists of stable localized structures separating the two orthogonal linear polarization eigenstates of the laser emission and is visible only when the total laser emission is measured. Numerical simulations based on the coupled complex Ginzburg-Landau equations have well reproduced the results of the experimental observation.

14.
Opt Express ; 17(17): 14767-70, 2009 Aug 17.
Article in English | MEDLINE | ID: mdl-19687954

ABSTRACT

We have demonstrated a Cs vapor laser with an unstable resonator transversely pumped by 15 narrowband laser diode arrays. A slope efficiency of 43%, a total optical efficiency of 31% and a maximum output power 49 W were obtained with a pump power of 157 Watts.

15.
J Nanosci Nanotechnol ; 9(2): 1190-3, 2009 Feb.
Article in English | MEDLINE | ID: mdl-19441485

ABSTRACT

A new structural combinatorial strategy toward efficient nanoscale structural optimization and direct nanophotonic and nanoelectronic device fabrication is introduced. The strategy was applied to develop a new multi-functional photodetector, which is able to simultaneously detect power, energy, and polarization of an incident UV light. The strategy was also used to study the dielectric behavior of ferroelectric relaxor PMN-PT heterophase superlattices in the terahertz (THz) frequencies in order to investigate their dielectric polariton properties and tunable dielectrics.

16.
Opt Express ; 17(9): 7361-7, 2009 Apr 27.
Article in English | MEDLINE | ID: mdl-19399114

ABSTRACT

This paper proposes a metallic hole array of a rectangular converging-diverging channel (RCDC) shape with extraordinary transmission. We use a three-dimensional (3D) finite element method to analyze the transmission characteristics of two-dimensional metallic hole arrays (2D-MHA) with RCDC. For a straight channel MHA, when the aperture size is reduced, the transmission peaks have a blue-shift. The same result is observed for a smaller gap throat for the RCDC structure. For the rectangular holes with a high length-width ratio, a similar blue-shift in the transmission peaks as well as a narrower full width at half maximum (FWHM) are observed. The asymmetry from the rectangular shape gives this structure high selectivity for light with different polarizations. Furthermore, the RCDC shape gives extra degrees of geometrical variables to 2D-MHA for tuning the location of the transmission peak and the FWHM. The tunable transmission property of this structure shows promise for applications in tunable filters, photonic circuits, and biosensors.


Subject(s)
Metals/chemistry , Refractometry/instrumentation , Computer-Aided Design , Equipment Design , Equipment Failure Analysis , Light , Refractometry/methods , Reproducibility of Results , Scattering, Radiation , Sensitivity and Specificity , Terahertz Radiation
17.
Opt Express ; 16(22): 17585-90, 2008 Oct 27.
Article in English | MEDLINE | ID: mdl-18958038

ABSTRACT

447.3 nm blue light generation was demonstrated through direct frequency doubling a continuous-wave Cesium vapor lasers 894.6 nm output using a PPKTP nonlinear crystal. The diode-pumped Cs vapor laser has an output power as large as 10 W with a very narrow emission linewidth less than 10 GHz. The PPKTP crystal is about 30 mm long and has a moderate acceptance wavelength bandwidth. The second harmonic wave generation efficiency achieved is about 4.4 %/W. Power depletion in second harmonic pulses, which relates to the absorption related thermal effects, was observed when using high pump power, long pulse duration, or high repetition rate.

18.
Opt Express ; 16(2): 748-51, 2008 Jan 21.
Article in English | MEDLINE | ID: mdl-18542151

ABSTRACT

We have demonstrated continuous wave operation of a laser diode array pumped Rb laser with an output power of 8 Watts. A slope efficiency of 60% and a total optical efficiency of 45% were obtained with a pump power of 18 Watts. This laser can be scaled to higher powers by using multiple laser diode arrays or stacks of arrays.


Subject(s)
Amplifiers, Electronic , Computer-Aided Design , Lasers , Lighting/instrumentation , Models, Theoretical , Rubidium , Semiconductors , Computer Simulation , Equipment Design , Equipment Failure Analysis , Gases , Lighting/methods
19.
Opt Lett ; 33(5): 414-5, 2008 Mar 01.
Article in English | MEDLINE | ID: mdl-18311276

ABSTRACT

Scaling of alkali lasers to higher powers requires using multiple diode lasers for pumping. The first (to our knowledge) results of a cw rubidium laser pumped by two laser diode arrays are presented. A slope efficiency of 53%, total optical efficiency of 46%, and output power of 17 W have been demonstrated.

20.
Opt Lett ; 32(18): 2692-4, 2007 Sep 15.
Article in English | MEDLINE | ID: mdl-17873937

ABSTRACT

The transmission of light through a thin Ag film with a periodic subwavelength hole array can be influenced by the presence of the externally applied magnetic field H. Using a three-dimensional finite element method, we show that the spectral locations of the transmission peak resonances can be shifted by varying the magnitude and direction of the H. The transmission peaks have blueshift, and the higher the magnitude of H the larger the blueshift. The shift is due to the change of cavity resonance condition as a result of the magneto-induced anisotropy in the optical properties of the Ag film. Hence, high transmittance for any desired wavelength can be achieved by applying an appropriate H to the metallic film of optimized material and hole parameters.

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