A narrow-bandwidth picosecond laser

D. Huppert; P. M. Rentzepis

doi:10.1063/1.90005

A narrow-bandwidth picosecond laser

D. Huppert^*, P. M. Rentzepis

^*Corresponding author for this work

Lucent

Research output: Contribution to journal › Article › peer-review

11 Scopus citations

Abstract

We have examined the advantages of using Nd³⁺/YAG as an amplifier for a ∼6 psec FWHM pulse generated by a mode-locked Nd ³⁺/glass oscillator. The Nd³⁺/glass oscillator pulse is characterized by 100 cm^-1 bandwidth at 1060 nm with variable temporal substructure. Passage of this pulse through a Nd³⁺/YAG rod resulted in wavelength-selected amplification of the specific Nd³⁺/YAG lines located within the envelope of the Nd/glass pulse. The result is a 100-fold amplified pulse consisting of two bands at 1061 nm and 1064 nm, each <3 cm^-1 in bandwidth with an average duration of 6 psec and as low as 4 psec.

Original language	English
Pages (from-to)	241-244
Number of pages	4
Journal	Applied Physics Letters
Volume	32
Issue number	4
DOIs	https://doi.org/10.1063/1.90005
State	Published - 1978
Externally published	Yes

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title = "A narrow-bandwidth picosecond laser",

abstract = "We have examined the advantages of using Nd3+/YAG as an amplifier for a ∼6 psec FWHM pulse generated by a mode-locked Nd 3+/glass oscillator. The Nd3+/glass oscillator pulse is characterized by 100 cm-1 bandwidth at 1060 nm with variable temporal substructure. Passage of this pulse through a Nd3+/YAG rod resulted in wavelength-selected amplification of the specific Nd3+/YAG lines located within the envelope of the Nd/glass pulse. The result is a 100-fold amplified pulse consisting of two bands at 1061 nm and 1064 nm, each <3 cm-1 in bandwidth with an average duration of 6 psec and as low as 4 psec.",

author = "D. Huppert and Rentzepis, \{P. M.\}",

year = "1978",

doi = "10.1063/1.90005",

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AU - Huppert, D.

AU - Rentzepis, P. M.

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N2 - We have examined the advantages of using Nd3+/YAG as an amplifier for a ∼6 psec FWHM pulse generated by a mode-locked Nd 3+/glass oscillator. The Nd3+/glass oscillator pulse is characterized by 100 cm-1 bandwidth at 1060 nm with variable temporal substructure. Passage of this pulse through a Nd3+/YAG rod resulted in wavelength-selected amplification of the specific Nd3+/YAG lines located within the envelope of the Nd/glass pulse. The result is a 100-fold amplified pulse consisting of two bands at 1061 nm and 1064 nm, each <3 cm-1 in bandwidth with an average duration of 6 psec and as low as 4 psec.

AB - We have examined the advantages of using Nd3+/YAG as an amplifier for a ∼6 psec FWHM pulse generated by a mode-locked Nd 3+/glass oscillator. The Nd3+/glass oscillator pulse is characterized by 100 cm-1 bandwidth at 1060 nm with variable temporal substructure. Passage of this pulse through a Nd3+/YAG rod resulted in wavelength-selected amplification of the specific Nd3+/YAG lines located within the envelope of the Nd/glass pulse. The result is a 100-fold amplified pulse consisting of two bands at 1061 nm and 1064 nm, each <3 cm-1 in bandwidth with an average duration of 6 psec and as low as 4 psec.

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A narrow-bandwidth picosecond laser

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