2015
DOI: 10.1117/12.2189455
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Delivery of ultrashort spatially focused pulses through a multimode fiber

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Cited by 1 publication
(5 citation statements)
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“…The experiments were conducted using a Ti:sapphire oscillator (Coherent Mira 900; central wavelength λ 𝑐 =800 nm; spectral width σ λ =10 nm; pulse width=100 fs). The capability of our method to form a sharp focused pulse through the fiber depends on the number of modes than can be controlled simultaneously [32]. In step-index fibers, the pulse spreading in time is given by: 𝜎 𝜏 ≈ 𝐿∆/(2𝑐 1 ) while in graded-index fibers: 𝜎 𝜏 ≈ 𝐿∆ 2 /(4𝑐 1 ) [36].…”
Section: Appendix A: Materials and Methodsmentioning
confidence: 99%
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“…The experiments were conducted using a Ti:sapphire oscillator (Coherent Mira 900; central wavelength λ 𝑐 =800 nm; spectral width σ λ =10 nm; pulse width=100 fs). The capability of our method to form a sharp focused pulse through the fiber depends on the number of modes than can be controlled simultaneously [32]. In step-index fibers, the pulse spreading in time is given by: 𝜎 𝜏 ≈ 𝐿∆/(2𝑐 1 ) while in graded-index fibers: 𝜎 𝜏 ≈ 𝐿∆ 2 /(4𝑐 1 ) [36].…”
Section: Appendix A: Materials and Methodsmentioning
confidence: 99%
“…The field emerging from the fiber on the proximal side is imaged by a 20x objective (OBJ1) and a 150 mm lens (L1) onto the CCD, where it is interfered by the pulsed reference beam. The pulsed reference can be delayed and is set at the time in which the visibility of the fringes is maximum [32].…”
Section: Appendix A: Materials and Methodsmentioning
confidence: 99%
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