Engineering of effective quadratic and cubic nonlinearities in two

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Engineering of effective quadratic and cubic nonlinearities in two-period QPM gratings
Bang, Ole; Clausen, Carl A. Balslev; Torner, L.
Published in:
Conference on Lasers and Electro-Optics
Link to article, DOI:
10.1109/CLEO.2000.906838
Publication date:
2000
Document Version
Publisher's PDF, also known as Version of record
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Citation (APA):
Bang, O., Clausen, C. A. B., & Torner, L. (2000). Engineering of effective quadratic and cubic nonlinearities in
two-period QPM gratings. In Conference on Lasers and Electro-Optics (pp. 147-148). OSA Technical Digest,
Optical Society of America. DOI: 10.1109/CLEO.2000.906838
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1-UEslIAY AFTERNOON / GLEU 2000 / %47
CTuA14
148 / CLEO 2000 / TUESDAY AFERNOON
IO.
11.
12.
0.Jlang~Y.S. Kivshar, A.V. liury;ik,A. Ik
Rossi, S. Trillo, "1wo~diiiieiision;iIsolitary wavcs in incilia with qu;alvatic i n i d
cubic iionlinearily," I'liys. I(cv. li 58,
5057 (IWS),
A. Kobyakiiv, I:. l,ederer, 0.liang, Y.S.
Kivshar, "N~i~iline;ir
phase shilt a t i d alloptical switching i n qiiasi-pli;iseInatchcd quadratic media," Opt. I.ctt. 23,
506 (1998).
0 . Bang, C , Ualslev (:lawen, 1'.1.. Cliristiansen, L. 'riiriier, "Engineering coiiipcliiig nonlinearities," Opt. l,etl. 24,
1413 (1999),
CTuA15
Generation of <4 cm-' transform
limited pulses in IR by difference
frequency mixing of stretched pulses
G,Veita.;, I<.
Iknielius. t:,, Schreiber,* r.nser
I~ecetircli(:eriier,
Viliiius Uwiv., .Siiiilet&io
Aveiiiie 9, l i i i i l r l i ~ i g3 , 2040 Viliiiiis, ~ ~ i t l r i i r r w i a ;
E-miiil: ~ e i l i i i ~ i i i u s . i ~ c i f rvii.11
ts~~//:
previous paper ivc h w c prcscntecl the
thcoictical background a n d experimental veriiication o( iiarriiw-b;indwi~Itli pulse generaLino via difkrcnce frequency iiiixiiig.l 'I'lic
tunahilily o l generated iiarrnw~I~andwidth
pulses wiis restricted to rather iiarrow wavelength r m g e in t1ieproxiriiityoll pin, w l i i c l i is
not olgseat plaLtical interest.
111thc present cimtribotion, we report 011
gcncrtition o f narrow-bandwidtli p u l s e s
within a 3-5 p i wavelength region that caii be
applied tci highly selective time-resnlved vi1il.ational spcctrmuq>y.
As a p u m p source we uscd a picosecond
'1i:Sappliire laser system delivering R O O - n m wavclcngtli I)iilscs with duration of 1.8 11s ,ind
energyof 1.5 i i i J , A p i s 1 ofthelases output was
trcquciicy douliled and used to plump a n oplic i i l par;nnetric gcnel.alor-ampl
which prodaced '- 1.3-lis pulses in (170-2600mil-wavclcngth ruigc. '%e idlcr witvc of the
Ol'O/A was used as a seed for subsequent diffcrcnic lrcqucncy (UP) iiiixinglparametric
aoiplificatinn p i i t i i p c d by 800-nm pulses.
111 the tirst series of expcrimcnts we generated the diflerence frequency in a cnnventional
r and seed pulses wcrc mixed in a
7-inn-thick K l ' A cryskil without stretching.
The VI' pulses that were pr"duccd llad a bandwidth of 12.3 ciii-'
I).
We memired duration of mipliiicd seed
pulse to he 1.2 1's (1:ig. 2). Crimptiter siiiiiiliition o l t h e prncess 11.1s slinwri that b ~ i t hUt:
pulsc and :~mplificdseed liave similar duration
wlicn p n p velocity mismatch is as sm;ill 'IS in
niir case. Witli tliisassuml,tionwc estiiniitc tlic
tiiiic~b;iodwidtliproduct d t h c 1R pulses t i i l i e
,-0.43, whicli is very close to t l i c time111our
L
12