High‐order Stokes and anti‐Stokes Raman generation in monoisotopic CVD  12 C‐diamond | Zendy

Kaminskii Alexander A. | Zendy; Lux Oliver | Zendy; Ralchenko Victor G. | Zendy; Bolshakov Andrey P. | Zendy; Rhee Hanjo | Zendy; Eichler Hans J. | Zendy; Shirakawa Akira | Zendy; Yoneda Hitoki | Zendy

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High‐order Stokes and anti‐Stokes Raman generation in monoisotopic CVD 12 C‐diamond

Author(s) -

Kaminskii Alexander A.,

Lux Oliver,

Ralchenko Victor G.,

Bolshakov Andrey P.,

Rhee Hanjo,

Eichler Hans J.,

Shirakawa Akira,

Yoneda Hitoki

Publication year - 2016

Publication title -

physica status solidi (rrl) – rapid research letters

Language(s) - English

Resource type - Journals

SCImago Journal Rank - 0.786

H-Index - 68

eISSN - 1862-6270

pISSN - 1862-6254

DOI - 10.1002/pssr.201600084

Subject(s) - raman spectroscopy , monoisotopic mass , raman scattering , picosecond , analytical chemistry (journal) , laser , diamond , materials science , crystal (programming language) , chemistry , optics , physics , chromatography , computer science , composite material , programming language , ion , organic chemistry

We determined, for the first time, the room temperature phonon energy related to the F 2g vibration mode ( ω SRS(12C) ∼ 1333.2 cm –1 ) in a mono‐crystalline single‐isotope CVD 12 C‐diamond crystal by means of stimulated Raman scattering (SRS) spectroscopy. Picosecond one‐micron excitation using a Nd 3+ :Y 3 Al 5 O 12 ‐laser generates a nearly two‐octave spanning SRS frequency comb (∼12000 cm –1 ) consisting of higher‐order Stokes and anti‐Stokes components. The spacing of the spectral lines was found to differ by Δ ω SRS ∼ 0.9 cm –1 from the comb spacing ( ω SRS(natC) ∼ 1332.3 cm –1 ) when pumping a conventional CVD diamond crystal with a natural composition of the two stable carbon isotopes 12 C (98.93%) and 13 C (1.07%). (© 2016 WILEY‐VCH Verlag GmbH &Co. KGaA, Weinheim)

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