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LETTERS Coherent control of optical information with matter wave dynamics Naomi S. Ginsberg
LETTERS Coherent control of optical information with matter wave dynamics Naomi S. Ginsberg

Non-reciprocal ultrafast laser writing
Non-reciprocal ultrafast laser writing

... produced in opposite directions, in other words with the writing direction along the 2y and þy axes of LiNbO3 , respectively (Fig. 1). We observed different material modifications depending on the pulse energy and the writing direction. With pulses energies below 1.4 mJ, a positive phase change (Dw) ...
253.pdf
253.pdf

crab cavity - Indico
crab cavity - Indico

Ab-Initio Calculations of Photonic Structures
Ab-Initio Calculations of Photonic Structures

Experimental Demonstration of Ground State Laser Cooling with
Experimental Demonstration of Ground State Laser Cooling with

Laser hazard control checklist
Laser hazard control checklist

workshop on laser-matter interaction 2010
workshop on laser-matter interaction 2010

Effect of input pulse chirp on nonlinear energy deposition and
Effect of input pulse chirp on nonlinear energy deposition and

Laser Bleaching of Carbon Nanotubes Suspension in
Laser Bleaching of Carbon Nanotubes Suspension in

recent advances - University of St Andrews
recent advances - University of St Andrews

Absorption Measurements in Microfluidic Devices using Ring-down Spectroscopy
Absorption Measurements in Microfluidic Devices using Ring-down Spectroscopy

Optically Pumped Solid-State Lasers
Optically Pumped Solid-State Lasers

... 8.6 The Nd:YAG Laser YAG has a combination of desirable properties as a host medium for Nd3+ ions: it has relatively high thermal conductivity, which allows it to disperse the waste heat from the optical pumping process; it has high mechanical strength, and can be grown as crystals of large size wit ...
Efficient  electromagnetically  induced  transparency COMMUNICATIONS
Efficient electromagnetically induced transparency COMMUNICATIONS

... by an amount equal to the repump field detuning, and there is asymmetric EIT on the two-photon resonance. which is in agreement with off resonant CPT measurements made in atomic beams [22]. For this data, the intensity of the coupling field is 90 W/cm’. We also studied EIT in Pr:YSO at higher tem~ra ...
The mechanism for continuum polarization in laser induced
The mechanism for continuum polarization in laser induced

Laser Bandwidth Measurements in Fiber Data Delivery for Corning
Laser Bandwidth Measurements in Fiber Data Delivery for Corning

... accordance with this standard can then be relied upon to perform in accordance with the standard. Sometimes, however, end-users may need a longer reach or need to use more connectors, and will seek out multimode fiber solutions that support their particular requirements. Such solutions place additio ...
Bose-Glass Phases of Ultracold Atoms due to Cavity Backaction Hessam Habibian,
Bose-Glass Phases of Ultracold Atoms due to Cavity Backaction Hessam Habibian,

Simultaneous Recovery of Two Ultrashort Laser
Simultaneous Recovery of Two Ultrashort Laser

A Practical Guide to Optical Trapping
A Practical Guide to Optical Trapping

Experimental realization of three-dimensional indefinite cavities at the nanoscale with
Experimental realization of three-dimensional indefinite cavities at the nanoscale with

Quantum State Engineering on an Optical Transition and
Quantum State Engineering on an Optical Transition and

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PDF

PubTeX output 2005.03.30:1333
PubTeX output 2005.03.30:1333

... by filling the central hole in a five-ring hexagonal lattice of air 0.45 , in a dielectric substrate [1]. The characholes with teristics of the cavity are and . This cavity exhibits resonance for several TM modes, including degenerated ones; for simplicity and without loss of generality, we as1 m. T ...
Revealing the time-dependent polarization of
Revealing the time-dependent polarization of

Synchronization of Micromechanical Oscillators Using Light
Synchronization of Micromechanical Oscillators Using Light

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Mode-locking



Mode-locking is a technique in optics by which a laser can be made to produce pulses of light of extremely short duration, on the order of picoseconds (10−12 s) or femtoseconds (10−15 s).The basis of the technique is to induce a fixed-phase relationship between the longitudinal modes of the laser's resonant cavity. The laser is then said to be 'phase-locked' or 'mode-locked'. Interference between these modes causes the laser light to be produced as a train of pulses. Depending on the properties of the laser, these pulses may be of extremely brief duration, as short as a few femtoseconds.
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