• Aucun résultat trouvé

Determination of the composition of heterogeneous binder solutions by surface plasmon resonance biosensing

N/A
N/A
Protected

Academic year: 2021

Partager "Determination of the composition of heterogeneous binder solutions by surface plasmon resonance biosensing"

Copied!
7
0
0

Texte intégral

(1)

Title

Determination of the composition of heterogeneous binder solutions by surface plasmon resonance biosensing

Authors

Jimmy Gaudreault, Benoît Liberelle, Yves Durocher, Olivier Henry*, Gregory De Crescenzo* *: These authors contributed equally to this work.

(2)

1. Supplementary Appendix A - Hessian matrix with 𝑵 analytes

The hessian matrix can be approximated by: 𝐻 ≈ ∑ ∑ (𝜕𝑅𝑇𝑂𝑇,𝑝𝑟𝑒𝑑 𝑠,𝑡 𝜕𝜽 ) 𝑇 (𝜕𝑅𝑇𝑂𝑇,𝑝𝑟𝑒𝑑 𝑠,𝑡 𝜕𝜽 ) 𝑇 𝑡=1 𝑆 𝑠=1 𝜽 = [𝒌𝒂′, 𝒌𝒅′ 𝑹𝒎𝒂𝒙′ , 𝑹𝑰′ ]′ With 𝜕𝑅𝑇𝑂𝑇,𝑝𝑟𝑒𝑑 𝜕𝜽 = ∑ 𝜕𝑅𝑝𝑟𝑒𝑑,𝑖 𝜕𝜽 𝑁 𝑖=1

The derivatives in (31) can be evaluated by solving the following ODEs along with the system of ODE in (6): 𝑑𝑹 𝑑𝑡 = 𝑓(𝑹, 𝜽) 𝑑 𝑑𝑡 𝑑𝑹 𝑑𝜽 = 𝜕𝒇 𝜕𝜽+ 𝜕𝒇 𝜕𝑹 𝜕𝑹 𝜕𝜽 𝑹(0) = [𝑅1(0), … 𝑅𝑁(0)]′ = [0, ⋯ ,0]′ 𝜕𝑹 𝜕𝜽|𝑡=0 = 0 𝑓𝑖 = 𝑘𝑎𝑖𝐹𝑖𝐶𝑇𝑂𝑇𝑅𝑚𝑎𝑥,𝑖(1 − ∑ 𝑅𝑗 𝑅𝑚𝑎𝑥,𝑗 𝑁 𝑗=1 ) − 𝑘𝑑𝑖𝑅𝑖 ∀ 𝑖 = 1, … , 𝑁

Here we present a way to compute the necessary gradient 𝜕𝑅𝑇𝑂𝑇,𝑝𝑟𝑒𝑑𝜕𝜽 to compute the hessian matrix related to the estimation of the kinetic parameters. Consider 3 matrices:

𝑿𝟏 = [ 𝜕𝑅1 𝜕𝑘𝑎,1 ⋯ 𝜕𝑅1 𝜕𝑘𝑎,𝑁 ⋮ ⋱ ⋮ 𝜕𝑅𝑁 𝜕𝑘𝑎,1 ⋯ 𝜕𝑅𝑁 𝜕𝑘𝑎,𝑁] = 𝜕𝑹 𝜕𝒌𝒂 𝑿𝟐= [ 𝜕𝑅1 𝜕𝑘𝑑,1 ⋯ 𝜕𝑅1 𝜕𝑘𝑑,𝑁 ⋮ ⋱ ⋮ 𝜕𝑅𝑁 𝜕𝑘𝑑,1 ⋯ 𝜕𝑅𝑁 𝜕𝑘𝑑,𝑁] = 𝜕𝑹 𝜕𝒌𝒅

(3)

𝑿𝟑 = [ 𝜕𝑅1 𝜕𝑅𝑚𝑎𝑥,1 ⋯ 𝜕𝑅1 𝜕𝑅𝑚𝑎𝑥,𝑁 ⋮ ⋱ ⋮ 𝜕𝑅𝑁 𝜕𝑅𝑚𝑎𝑥,1 ⋯ 𝜕𝑅𝑁 𝜕𝑅𝑚𝑎𝑥,𝑁] = 𝜕𝑹 𝜕𝑹𝒎𝒂𝒙 With 𝑹 = [𝑅1, ⋯ 𝑅𝑁]′.

Sensibility with respect to 𝒌𝒂,𝒊 :

𝑑𝑿𝟏 𝑑𝑡 (𝑖, 𝑖) = 𝜕𝑓𝑖 𝜕𝑘𝑎,𝑖 + 𝜕𝑓𝑖 𝜕𝑅𝑖 ∗ 𝜕𝑅𝑖 𝜕𝑘𝑎,𝑖 + ∑𝜕𝑓𝑖 𝜕𝑅𝑗 ∗ 𝜕𝑅𝑗 𝜕𝑘𝑎,𝑖 𝑁 𝑗≠𝑖 = 𝜕𝑓𝑖 𝜕𝑘𝑎,𝑖 + 𝜕𝑓𝑖 𝜕𝑅𝑖 ∗ 𝑋1(𝑖, 𝑖) + ∑ 𝜕𝑓𝑖 𝜕𝑅𝑗 ∗ 𝑋1(𝑗, 𝑖) 𝑁 𝑗≠𝑖 𝑑𝑿𝟏 𝑑𝑡 (𝑖, 𝑗) = 𝜕𝑓𝑖 𝜕𝑘𝑎,𝑗 + 𝜕𝑓𝑖 𝜕𝑅𝑖 ∗ 𝜕𝑅𝑖 𝜕𝑘𝑎,𝑗 + ∑ 𝜕𝑓𝑖 𝜕𝑅𝑘 ∗ 𝜕𝑅𝑘 𝜕𝑘𝑎,𝑗 𝑁 𝑘≠𝑖 = 𝜕𝑓𝑖 𝜕𝑘𝑎,𝑗 + 𝜕𝑓𝑖 𝜕𝑅𝑖 ∗ 𝑋1(𝑖, 𝑗) + ∑ 𝜕𝑓𝑖 𝜕𝑅𝑘 ∗ 𝑋1(𝑘, 𝑗) 𝑁 𝑘≠𝑖

With partial derivatives:

𝜕𝑓𝑖 𝜕𝑅𝑖 = −𝑘𝑎,𝑖𝐹𝑖𝐶𝑇𝑂𝑇− 𝑘𝑑,𝑖 𝜕𝑓𝑖 𝜕𝑅𝑗 = −𝑘𝑎,𝑖𝐹𝑖𝐶𝑇𝑂𝑇 𝑅𝑚𝑎𝑥,𝑖 𝑅𝑚𝑎𝑥,𝑗 𝜕𝑓𝑖 𝜕𝑘𝑎,𝑖 = 𝐹𝑖𝐶𝑇𝑂𝑇𝑅𝑚𝑎𝑥,𝑖(1 − ∑ 𝑅𝑗 𝑅𝑚𝑎𝑥,𝑗 𝑁 𝑗=1 ) 𝜕𝑓𝑖 𝜕𝑘𝑎,𝑗 = 0 We obtain:

(4)

𝜕𝑅𝑃𝑅𝐸𝐷,𝑇𝑂𝑇 𝜕𝒌𝒂 = [ ∑ 𝜕𝑅𝑖 𝜕𝑘𝑎1 𝑁 𝑖=1 ⋮ ∑ 𝜕𝑅𝑖 𝜕𝑘𝑎𝑁 𝑁 𝑖=1 ] = [ 𝜕𝑅𝑃𝑅𝐸𝐷,𝑇𝑂𝑇 𝜕𝑘𝑎1 ⋮ 𝜕𝑅𝑃𝑅𝐸𝐷,𝑇𝑂𝑇 𝜕𝑘𝑎𝑁 ]

Sensibility with respect to 𝒌𝒅,𝒊 :

𝑑𝑿𝟐 𝑑𝑡 (𝑖, 𝑖) = 𝜕𝑓𝑖 𝜕𝑘𝑑,𝑖 + 𝜕𝑓𝑖 𝜕𝑅𝑖 ∗ 𝜕𝑅𝑖 𝜕𝑘𝑑,𝑖 + ∑𝜕𝑓𝑖 𝜕𝑅𝑗 ∗ 𝜕𝑅𝑗 𝜕𝑘𝑑,𝑖 𝑁 𝑗≠𝑖 = 𝜕𝑓𝑖 𝜕𝑘𝑑,𝑖+ 𝜕𝑓𝑖 𝜕𝑅𝑖∗ 𝑋2 (𝑖, 𝑖) + ∑𝜕𝑓𝑖 𝜕𝑅𝑗∗ 𝑋2(𝑗, 𝑖) 𝑁 𝑗≠𝑖 𝑑𝑿𝟐 𝑑𝑡 (𝑖, 𝑗) = 𝜕𝑓𝑖 𝜕𝑘𝑑,𝑗 + 𝜕𝑓𝑖 𝜕𝑅𝑖 ∗ 𝜕𝑅𝑖 𝜕𝑘𝑑,𝑗 + ∑ 𝜕𝑓𝑖 𝜕𝑅𝑘 ∗ 𝜕𝑅𝑘 𝜕𝑘𝑑,𝑗 𝑁 𝑘≠𝑖 = 𝜕𝑓𝑖 𝜕𝑘𝑑,𝑗 + 𝜕𝑓𝑖 𝜕𝑅𝑖 ∗ 𝑋2(𝑖, 𝑗) + ∑ 𝜕𝑓𝑖 𝜕𝑅𝑘 ∗ 𝑋2(𝑘, 𝑗) 𝑁 𝑘≠𝑖

With partial derivatives:

𝜕𝑓𝑖 𝜕𝑘𝑑,𝑖 = −𝑅𝑖 𝜕𝑓𝑖 𝜕𝑘𝑑,𝑗 = 0 We obtain: 𝜕𝑅𝑃𝑅𝐸𝐷,𝑇𝑂𝑇 𝜕𝒌𝒅 = [ ∑ 𝜕𝑅𝑖 𝜕𝑘𝑑1 𝑁 𝑖=1 ⋮ ∑ 𝜕𝑅𝑖 𝜕𝑘𝑑𝑁 𝑁 𝑖=1 ] = [ 𝜕𝑅𝑃𝑅𝐸𝐷,𝑇𝑂𝑇 𝜕𝑘𝑑1 ⋮ 𝜕𝑅𝑃𝑅𝐸𝐷,𝑇𝑂𝑇 𝜕𝑘𝑑𝑁 ]

(5)

Sensibility with respect to 𝑹𝒎𝒂𝒙,𝒊 : 𝑑𝑿𝟑 𝑑𝑡 (𝑖, 𝑖) = 𝜕𝑓𝑖 𝜕𝑅𝑚𝑎𝑥,𝑖 + 𝜕𝑓𝑖 𝜕𝑅𝑖 ∗ 𝜕𝑅𝑖 𝜕𝑅𝑚𝑎𝑥,𝑖 + ∑𝜕𝑓𝑖 𝜕𝑅𝑗 ∗ 𝜕𝑅𝑗 𝜕𝑅𝑚𝑎𝑥,𝑖 𝑁 𝑗≠𝑖 = 𝜕𝑓𝑖 𝜕𝑅𝑚𝑎𝑥,𝑖 +𝜕𝑓𝑖 𝜕𝑅𝑖 ∗ 𝑋3(𝑖, 𝑖) + ∑ 𝜕𝑓𝑖 𝜕𝑅𝑗 ∗ 𝑋3(𝑗, 𝑖) 𝑁 𝑗≠𝑖 𝑑𝑿𝟑 𝑑𝑡 (𝑖, 𝑗) = 𝜕𝑓𝑖 𝜕𝑅𝑚𝑎𝑥,𝑗+ 𝜕𝑓𝑖 𝜕𝑅𝑖∗ 𝜕𝑅𝑖 𝜕𝑅𝑚𝑎𝑥,𝑗+ ∑ 𝜕𝑓𝑖 𝜕𝑅𝑘∗ 𝜕𝑅𝑘 𝜕𝑅𝑚𝑎𝑥,𝑗 𝑁 𝑘≠𝑖 = 𝜕𝑓𝑖 𝜕𝑅𝑚𝑎𝑥,𝑗 +𝜕𝑓𝑖 𝜕𝑅𝑖 ∗ 𝑋3(𝑖, 𝑗) + ∑ 𝜕𝑓𝑖 𝜕𝑅𝑘 ∗ 𝑋3(𝑘, 𝑗) 𝑁 𝑘≠𝑖

With partial derivatives:

𝜕𝑓𝑖 𝜕𝑅𝑚𝑎𝑥,𝑖 = 𝑘𝑎,𝑖𝐹𝑖𝐶𝑇𝑂𝑇(1 − ∑ 𝑅𝑗 𝑅𝑚𝑎𝑥,𝑗 𝑁 𝑗≠𝑖 ) 𝜕𝑓𝑖 𝜕𝑅𝑚𝑎𝑥,𝑗 =𝑘𝑎,𝑖𝐹𝑖𝐶𝑇𝑂𝑇𝑅𝑚𝑎𝑥,𝑖 𝑅𝑚𝑎𝑥,𝑗2 𝑅𝑗 We obtain: 𝜕𝑅𝑃𝑅𝐸𝐷,𝑇𝑂𝑇 𝜕𝑅𝑚𝑎𝑥 = [ ∑ 𝜕𝑅𝑖 𝜕𝑅𝑚𝑎𝑥,1 𝑁 𝑖=1 ⋮ ∑ 𝜕𝑅𝑖 𝜕𝑅𝑚𝑎𝑥,𝑁 𝑁 𝑖=1 ] = [ 𝜕𝑅𝑃𝑅𝐸𝐷,𝑇𝑂𝑇 𝜕𝑅𝑚𝑎𝑥,1 ⋮ 𝜕𝑅𝑃𝑅𝐸𝐷,𝑇𝑂𝑇 𝜕𝑅𝑚𝑎𝑥,𝑁 ]

(6)

𝜕𝑅𝑃𝑅𝐸𝐷,𝑇𝑂𝑇 𝜕𝜽 = [ 𝜕𝑅𝑃𝑅𝐸𝐷,𝑇𝑂𝑇 𝜕𝑘𝑎1 ⋮ 𝜕𝑅𝑃𝑅𝐸𝐷,𝑇𝑂𝑇 𝜕𝑘𝑎𝑁 𝜕𝑅𝑃𝑅𝐸𝐷,𝑇𝑂𝑇 𝜕𝑘𝑑1 ⋮ 𝜕𝑅𝑃𝑅𝐸𝐷,𝑇𝑂𝑇 𝜕𝑘𝑑𝑁 𝜕𝑅𝑃𝑅𝐸𝐷,𝑇𝑂𝑇 𝜕𝑅𝑚𝑎𝑥,1 ⋮ 𝜕𝑅𝑃𝑅𝐸𝐷,𝑇𝑂𝑇 𝜕𝑅𝑚𝑎𝑥,𝑁 ]

Which enables the computation of the gradient 𝜕𝑅𝑇𝑂𝑇,𝑝𝑟𝑒𝑑

𝜕𝜽 . Computing this gradient at every time

(7)

2. Supplementary Appendix B - Confidence intervals on the fractions

We define 𝐹̂𝑖 as the estimated fraction of analyte 𝑖, i.e.:

𝜽̂ = [ 𝐹̂1

⋮ 𝐹̂𝑁

]

We propose an algorithm similar to the bisection method. Pose: 𝐺(𝐹𝑖0) = 𝐽(𝜃)|𝐹𝑖=𝐹𝑖0− 𝐽(𝜃̂) − 𝐹1−𝛼(1, 𝑛 − 𝑝) ∗

𝑛 − 𝑝 𝐽(𝜃̂)

The boundary of the confidence interval is such that 𝐺(𝐹𝑖0) = 0. If points 𝑎 and 𝑏 such that

𝐺(𝑎) > 0 and 𝐺(𝑏) < 0 are known, the algorithm consists in: 1. Compute 𝐺 (𝑎+𝑏2 ).

2. If 𝐺 (𝑎+𝑏2 ) < 0, pose 𝑏 =𝑎+𝑏

2 . Otherwise, pose 𝑎 = 𝑎+𝑏

2 .

3. Test for convergence, i.e. the algorithm can be stopped if 𝑎 − 𝑏 < 𝑇𝑂𝐿 or if 𝑎+𝑏2 is such that 𝐹𝑖0> 1 in the case of an upper bound or 𝐹𝑖0< 0 in the case of a lower bound.

4. If there is convergence, the boundary is given by 𝐹̂𝑖+𝑎+𝑏2 in the case of an upper bound

or 𝐹̂𝑖− 𝑎+𝑏

2 in the case of a lower bound. Otherwise, return to step 1.

5. Repeat for every analyte and for upper and lower bounds. To obtain starting points for 𝑎 and 𝑏, we can:

1. Pose 𝑎 = 0.5% and 𝑏 = 0%. 2. Compute 𝐺(𝑎).

3. If 𝐺(𝑎) < 0, pose 𝑏 = 𝑎, double 𝑎 then return to step 2.

4. If 𝐺(𝑎) > 0, the current 𝑎 and 𝑏 can be used as a starting point for the bisection algorithm.

Références

Documents relatifs

Its use in detection of the defects, particularly in the determination of corrosions .The contained information in the received signal makes it possible to determine

Optimum coupling between the incident light and the surface Plasmon wave (surface plasmon resonance condition) is strongly dependent on the refractive index

The data that support the plots within this paper and other findings of this study are available in the main text and Extended Data Figures. Additional information is available

Effect of the TA concentration in the reducing solution on AuNPs size; Calculation of AuNPs concentration; Calculation to deter- mine the added Ag content for dedicated shell

In this study, the optimization of the two parameters e 1 and e 2 is made with Nelder-Mead algorithm. Nevertheless, we have verified the results that could depend on the starting

Since the number of memory blocks in use at any given time is bounded by the size of the address space (and often in practice by a significantly stricter bound), timely reclaiming

Technical Note (National Research Council of Canada. Division of Building Research), 1969-09-26.. READ THESE TERMS AND CONDITIONS CAREFULLY BEFORE USING THIS

After the transition to temperate climates in the late Eocene, we found that diversification rates of turtles, crocodiles, and lepi- dosaurs living in temperate climatic conditions