V. Perina et al., RBS MEASUREMENT OF DEPTH PROFILES OF ERBIUM INCORPORATED INTO LITHIUM-NIOBATE FOR OPTICAL AMPLIFIER APPLICATIONS, Nuclear instruments & methods in physics research. Section B, Beam interactions with materials and atoms, 139(1-4), 1998, pp. 208-212
Rutherford Backscattering Spectrometry (RBS) was used for the determin
ation of Er3+ concentration profiles in locally doped lithium niobate.
The doped layers are the basic substrates for the fabrication of opti
cal waveguiding structures which may be utilized as planar optical amp
lifiers and waveguiding lasers making use of the I-4(13/2) --> I-4(15/
2) transition in Er3+ which falls into the third low loss telecommunic
ation window (1.5 mu m). We present a new aproach of fabrication of lo
cally doped lithium niobate single crystal wafers. The doping occurs u
nder moderate temperature (similar to 350 degrees C) from reaction mel
ts containing ca. 10 wt% of erbium nitrate, The erbium content in part
icular cuts varies dramatically between ca. 3 at.% in the Y- and Z-cut
up to 20 at.% in the X-cuts. Erbium ions are localized in a 50 nm thi
ck layer, but they can be diffused deeper into the substrate by subseq
uent annealing at 350 degrees C. The Er concentrations of the samples
doped at moderated temperature are compared with the Er concentrations
of the samples doped by a standard high-temperature diffusion (> 1000
degrees C) from evaporated metal layers. To utilize the Er doped subs
trates in integrated optic circuits high quality waveguides must be su
bsequently fabricated. For that we used the Annealed Proton Exchange (
APE) method with adipic acid. For the actual fabrication of the wavegu
ides the following order of operation should be kept: the erbium dopin
g should be done before the APE because the substantially changed stru
cture of APE layers prevents the doping process. The APE process is ch
ecked by measurements of lithium depth profiles by Neutron Depth Profi
ling (NDP). (C) 1998 Elsevier Science B.V.