2016
DOI: 10.1364/boe.8.000315
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Compact diode laser source for multiphoton biological imaging

Abstract: Abstract:We demonstrate a compact, pulsed diode laser source suitable for multiphoton microscopy of biological samples. The center wavelength is 976 nm, near the peak of the two-photon cross section of common fluorescent markers such as genetically encoded green and yellow fluorescent proteins. The laser repetition rate is electrically tunable between 66.67 kHz and 10 MHz, with 2.3 ps pulse duration and peak powers >1 kW. The laser components are fiber-coupled and scalable to a compact package. We demonstrate … Show more

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Cited by 11 publications
(4 citation statements)
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“…To determine the orientation of PGS and PLGA within the nanofibers, we developed a method to investigate this using Raman imaging [ 36 ]. Through confocal Raman spectroscopy of single fiber strands, it was previously confirmed that the 1.5/1.5/11/15 core/shell electrospinning configuration obtained specific chemical composition signatures of PGS in the core and PLGA in the shell [ 36 ].…”
Section: Resultsmentioning
confidence: 99%
“…To determine the orientation of PGS and PLGA within the nanofibers, we developed a method to investigate this using Raman imaging [ 36 ]. Through confocal Raman spectroscopy of single fiber strands, it was previously confirmed that the 1.5/1.5/11/15 core/shell electrospinning configuration obtained specific chemical composition signatures of PGS in the core and PLGA in the shell [ 36 ].…”
Section: Resultsmentioning
confidence: 99%
“…Efficiency of multiphoton processes is influenced by (i) focalization characteristics, (ii) characteristics of the biological sample imaged and (iii) excitation source and its parameters. A theory considered as a reference for the comparison of sources for MPM is precisely described by Webb et al [2,14,51], and is regularly recalled for pulsed lasers [9,16,135,136,138,144], in the case of mode-locked systems or alternative technologies. This evaluation is based either on the estimation of the number of photons emitted by TPF or on the number of photons absorbed by TPA.…”
Section: Theoretical Elements Of Laser Source Comparisonmentioning
confidence: 99%
“…Besides, the core diameter of fiber employed in this demonstration was ~21 um, suggesting only ~300 um 2 fundamental mode (FM) field area. Moreover, such long cavity lengths are not desirable for high peak power ultrafast lasers at 976 nm [12,13], which find application in two-photon microscopy [14] and frequency conversion to 488 nm in crystals [13]. To achieve high efficiency ultrafast lasing, it is highly desirable to have an effectively singlemoded, large mode area YDF that inherently possesses high differential loss at four-level lasing wavelengths.…”
Section: Introductionmentioning
confidence: 99%