HAL Id: hal-01891918
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Submitted on 18 Oct 2018
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Toward hybrid polymer-porous silicon waveguides for
Vernier-effect optical biosensors
Paul Azuelos, Nathalie Lorrain, M. Guendouz, Parastesh Pirasteh, Jonathan
Lemaitre, Isabelle Hardy, Joël Charrier, Monique Thual
To cite this version:
Paul Azuelos, Nathalie Lorrain, M. Guendouz, Parastesh Pirasteh, Jonathan Lemaitre, et al.. Toward hybrid polymer-porous silicon waveguides for Vernier-effect optical biosensors. 11th Porous Semicon-ductors - Science and Technology 2018 Conference (PSST 2018), Mar 2018, La Grande Motte, France. �hal-01891918�
Toward hybrid Polymer-Porous silicon waveguides
for Vernier effect optical biosensors
P.Azuelos
a
, N.Lorrain
a
, M.Guendouz
a
, P.Pirasteh
a
,J.Lemaître
a
,
I.Hardy
b
,J.Charrier
a
and M.Thual
a
a
UMR FOTON, Université de Rennes 1, France
b
UMR FOTON, IMT Atlantique, France
Introduction on integrated MR
•
Microresonator sensing
τ
τ'
κ
κ'
E
iE
tFWHM
λ
resFSR
Δλ
res|T(
λ
)|
2λ
no analytes
presence of analytes
R
Lc
Sensor performance evaluation with
Sensitivity and
Limit of Detection :
S =
∆λ
res
∆C
analytes
LOD =
N oises
S
Main economic field : Health, Research, Industrie,
Biodefense, Environnemental
•
PSi for surface sensing
Bulk
core
Bulk
cladding
Substrate
Grafted
molecules
EM
Field
Porous
core
Porous
cladding
Evanescent detection
Volume detection
PSi advantage : High sensing sensitivity
Bulk material advantage : Low propagation losses
Porous silicon MR fabrication
•
Thermal treatment of PSi
Partial oxidation remove native hydrophobicity,
im-prove PSi layers stability in time and tune RI
•
Photolithography and etching
UV exposure
development
of photoresist
dry etching
of core waveguide
Photoresist resin
Core
Optical confinment layer
Si-Substrate
Core
Si-Substrate
Si-Substrate
Optical confinment layer Optical confinment layer
Ion bombardment
Insolation
of photoresist
solvant
•
PSi MR sensor
P+ Boron doped Si (5mΩ.cm
−1
) ; Current density
applied : (Core/Cladding) (
50/80) mA.cm
−2
; HF sol.
prop. HF(50%)/ethanol/water :
2:2:1.
Sensor characterisation
•
Experimental setup
Fiber-waveguide coupling
with microlens
Peltier thermostat
Sample
Tunable laser
Tin λi(t) wavelength scanPower-meter
λλi(t)
T
out λ•
PSi MR homogeneous sensitivity
cha-racterisation
Optimization of ridge PSi waveguides dimensions
Losses evaluation in PSi waveguides
•
Choice of PSI porosity and
oxidation rate
nonox
300°C
500°C
750°C
850°C
oxydationCurrent density (mA.cm-2)
10 30 50 100
Electropolishing
Full pore filling
after oxidation
Low current
density
0 0 0 0.1 0.1 0.1 0.2 0.2 0.2 0.3 0.3 0.3 0.4 0.4 0.4 0.5 0.5 0.5 0.6 0.6 0.6 0.7 0.7 0.7 0.8 0.8 0.8 0.9 0.9 0.9 1 1 1f
airf
Sif
Si0 2 Studied oxidation (500°C(1h)) - fsiO2<30% - no hydrophobicity2
SD1
SDn
coren
claddingΔn
0.16 0.54 1.35 1.35 1.51 1.89 (RIU)•
Determination of losses with
waveguide dimensions
10
1
SD2
SD4
3.5
3
2.5
2
1.5
1
0.5
0
0
0.5
1
1.5
2
2.5
3
3.5 4
Overall Losses TE00
Surface Detection
dB/cm
Width (μm)
Heigth (
μ
m
)
5
15
20
25
30
35
40
Sensitivity and Limit of detection
•
Sensitivity of PSi MR
1
SD2
SD4
3.5
3
2.5
2
1.5
1
0.5
0
0
0.5
1
1.5
2
2.5
3
3.5 4
Sensitivity TE00
nm/(pg.mm-2)
0.02
0.025
0.03
0.04
Width (μm)
Heigth (
μ
m
)
0.035
•
Limit of detection
4
3.5
3
2.5
2
1.5
1
0.5
0
0
0.5
1
1.5
2
2.5
3
3.5 4
LOD TE00
pg.mm-2
0
0.5
1
1.5
2
2.5
3
3.5
Width (μm)
Heigth (
μ
m
)
4
Optimized performances :
S=0.04 nm/(pg.mm
−2
)
LOD=0.5 pg.mm
−2
Toward hybrid Vernier effect
Vernier effect : Cascaded micro-resonators
T
sens
λ
TinOne micro-resonator
λ
T
sens
Ligth input
Ligth output
T
refT
sensT
ref.T
sensSU8 waveguide
PSi waveguide
adiabatic taper
reference
Micro-resonator
Analytes sensitive Micro-resonatorλ
Tin 100 μmSU8
waveguide
PSi waveguide
MEB illustration of hybrid
polymer-PSi MR
Sensitivity : ×10
3
LOD : ÷10
2
Vernier effect can improve sensor performances
with a reference interferometer
Conclusion and Perspective
•
MR integrated sensor sensitivity and
LOD
0.01
0.1
1
10
100
1E-5
1E-4
1E-3
0.01
0.1
1
10
bulk ridge MR (exp)
bulk slot MR (exp)
PSi MR (sim)
Hybrid PSi-Polymer Vernier (sim)
S
e
ns
itiv
ity
(
nm/
(
pg.mm
-2
))
Limit of detection (pg.mm-2)
[1]
[*]
[4]
[3]
[6]
[5]
[2]
* Simple PSi MR[1] P.Azuelos & al. JAP 121 144501 (2017) [2] C.F.Carlborg & al. Lab on CHip 10(3) (2010)
[3] M.S.Luchansky & al. Biosens. & Bioelec. 26(4) (2010) [4] K.D.Vos & al. Opt. Exp. 15(12) (2007)
[5] C.A.Barrios & al. Opt. Lett. 33(7) (2008) [6] K.D.Vos & al. Biosens. & Bioelec. 24(8) (2009)