Title: Room temperature operation of epitaxial leadtelluride detectors monolithically integrated on midinfr
1Room temperature operation of epitaxial
lead-telluride detectors monolithically
integrated on midinfrared filters
- M. Böberl, T. Schwarzl, J. Roither, T. Fromherz,
G. Springholz and W. Heiss - Institut für Halbleiter- und Festkörperphysik,
- Universität Linz, Österreich
- Outline
- Introduction and Motivation
- Room temperature photoconductivity from PbTe
epilayers - Integrated narrow-band photovoltaic detectors for
room temperature operation - Conclusion
2Compact uncooled sensor systems
- Detection of hydrocarbons or CO2 in ambient air
via IR transmission measurements - optical prerequisites
- - broad IR source
- 2 broadband detectors and 2 narrow-band
interference filters - first filter wavelength coincides with certain
molecule absorption line, used for the measuring
detector - second one is off resonance and is used for the
reference detector - c monolithic integration of filter and detector
for more compact systems
DraegerSensors IR Ex HC-68 08 475
3Applications of IR monitoring systems
e.g. early warning of potentially explosive
hydrocarbon levels. These devices are used in a
wide variety of industrial facilities and are an
integral part of plant safety systems.
- all hydrocarbons have the characteristic C-H
stretch which occurs between 3100 and 2850 cm-1 - alcohols and amines display strong broad O-H and
N-H stretching bands in the region 3400 to 3100
cm-1 - alkene and alkyne C-H bonds display sharp
stretching absorptions in the region 3100 to 3000
cm-1 - triple bond stretching absorptions occur in the
region 2400 to 2200 cm-1
c 3 to 4.5 mm wavelength region favorable
4Polycrystalline PbSe Photodetectors
Room temperature detectivities of 1.8 x 1010
cmHz½W-1 at 3.8 mm
Response times some ms
fabrication film deposition by thermal
evaporation baking process for sensitization to
infrared radiation
5Monolithically Integrated Polycrystalline PbSe
Photodetectors
J. Diezhandino, APL 83, 2751 (2003) Monolithic
integration of spectrally selective uncooled lead
selenide detectors for low cost applications
filter structure 50 layers Ge/SiO
experiment
simulation
c baking for sensitization is limited by thermal
stability of the filter structure
band pass
6Monolithic integration of epitaxial
lead-telluride photodetectors
- PbTe narrow gap semiconductor, high index of
refraction n, - EuTe wide gap semicond., low n
- Pb1-xEuxTe completely miscible alloy system
with very large band gap tunability - lattice mismatch between
- Pb1-xEuxTe/EuTe lt 2
- good matching of thermal expansion coefficients
(PbTe 19.8x106K-1, EuTe 13.6x106K-1, BaF2
19.8x106K-1) - high refractive index contrast of Dn/n80 c
efficient interference mirrors and filters
c filter structures of Pb1-xEuxTe/EuTe layers
photosensitive PbTe layer
7Room temperature photoconductivity from PbTe
epilayers grown on l/4 antireflection layers
Experimental setup and sample description
S1 1 mm thick PbTe grown on a l/4 EuTe
antireflection coating R1 single 2.5 mm PbTe
epilayer
- Reflectivity spectra
- S1 shows a pronounced minimum in reflectivity at
3.1 mm due to l/4 EuTe antireflection layer - RT photoconductivity spectra measured at a bias
of 1 mA - S1 shows a broad maximum at 3.1 mm c complies
with distinct minimum in reflectivity spectrum - Spectra obtained by forward biasing (lines) and
reverse biasing (symbols) match perfectly c pure
photoconductivity
8Responsivity at room temperature
- measured with a HeNe-laser at 3.36 mm and a
power of 5 mW
at a bias of 1 mA R1 Rl 1.4 V/W S1 -
illumination through EuTe antireflection layer
c Rl 2.9 V/W- direct illumination of the
PbTe layer c Rl 1.29 V/Wc enhancement of
responsivity by 2.2 in agreement with the ratio
of reflectivites (1-Rbackside)/(1-Rfrontside)
9Device characteristics
Noise voltage per band width un/(Df)1/2 22
nV/Hz½ measured with 300 K background radiation
at 10 kHz and a bias of 1 mA
8 ms
- Detectivity calculated from
- DRl(ADf) ½ /un
- room temperature detectivity at a bias of 1 mA
1.36x107 cmHz½W-1 - small compared to polycrystalline detectors
- studying possibility to obtain room temperature
photoresponse from photovoltaic devices
4 ms
- Response times
- measured at l 800 nm
- rise times smaller than 8 ms
- comparable with those of polycrystalline lead
salt detectors
10Integrated PbTe photodetectors on
narrow-bandwidth filters
Design for 3.6 mm and room temperature
filter consisting of - 2 Bragg mirrors with 1
and 1.5 PbEuTe/EuTe mirror pairs, high
refractive index contrast of mirror layers c
reflectivity of mirrors is 83 - in between
l/2 thick PbEuTe layer c cavity resonance at 3.6
mm active layer 500 nm thick p-PbTe with 1x1017
cm-3 p-type contact Pt/Ti/Au on PbTe
n-type contact In on EuTe
11Characteristics of integrated PbTe photodetectors
photosensitive PbTe layer
1 mm
EuTe/Pb0.94Eu0.06Te top Bragg mirror
l/2 cavity
bottom Bragg mirror
mid-IR transparent BaF2 substrate
c one narrow resonance peak
12Photovoltaic response of integrated PbTe
photodetectors
- one single peak at
- 3.66 mm with a linewidth of 100 nm
- Dl/l 2.7
- photovoltage peak coincides with that in
transmittance in both, position and linewidth - broad band at l lt 3 mm can be inhibited
13Conclusions
- Demonstration of room temperature
photoconductivity as well as photovoltaic
operation of epitaxial PbTe detectors - Monolithically integration of photosensitive PbTe
layers with EuTe/PbEuTe midinfrared filters - PbTe detectors grown on l/4 antireflection layers
c more than doubling of the responsivity - Integration of PbTe detectors with microcavities
acting as efficient narrow band filters c one
single resonance in the photoresponse with a Dl/l
of 2.7 in coincidence with OC-H stretching bond
Outlook Improved photovoltaic response by
extrinsically doped EuTe
Acknowledgements
G. Pillwein for SEM, bmbwk, FWF (START-Projekt
Y179 and SFB IR-ON), GME