| nextnano3 - Tutorialnext generation 3D nano device simulator1D TutorialISFET (Ion-Selective Field Effect Transistor): Si-SiO2 electrolyte sensorAuthor:
Stefan Birner If you want to obtain the input file that is used within this tutorial, please 
submit a support ticket.
 -> 1DSi_SiO2_electrolyte_sensor.in        
-
Loop over pH values from pH = 0 to pH = 14.pH = 6.4-> 1DSi_SiO2_electrolyte_sensor_pH64.in   -
 This tutorial is based on the diploma thesis of Michael Bayer, TU Munich 
(2004). Acknowledgement: The author - Stefan Birner - would like to thank 
Christian Uhl and Michael Bayer for helping to include the electrolyte features into nextnano³. 
 Si-SiO2 electrolyte sensorHere, we predict the sensitivity of electrolyte 
gate Si-SiO2 sensors to pH values of the electrolyte solution that 
covers the semiconductor structure.The charge density due to chemical reactions at the oxidic 
semiconductor-electrolyte interface is described within the site-binding model (
 $interface-states).We calculate the spatial charge and potential distribution both in the 
semiconductor and the electrolyte (Poisson-Boltzmann equation) 
self-consistently.
 The Si-SiO2 sensor that is exposed to an electrolyte solution has the 
following schematic layout: 
 
 Fig. 1: Si-SiO2 sensor with electrolyte gate.
 We simulate the structure along the z direction 
so that the structure is effectively 
one-dimensional, i.e. laterally homogeneous.The heterostructure is assumed to be grown along the [001] 
direction and is not strained.
 The file 
densities/interface_densitiesD.txt gives us information about the 
relevant interface charge densities: 
  Interface 4 (1544 nm): Interface charge sigmaadsorbed that 
  results from the site-binding model that describes chemical reactions at the 
  oxidic semiconductor-electrolyte interface. More details: 
  $interface-states
  $interface-statestotal 
  density of surface sites, i.e. surface hydroxyl groupsstate-number          =
  1          
  ! between SiO2 / Electrolyte at 1544 nm
 state-type            
  = electrolyte ! 
  sigma_adsorbed
 interface-density     = 5.0d14     
  ! [cm^-2] -
concentration inadsorption-constant   = 0.079433d0 
  ! K1 = adsorption   constant = 1 * 
  10-1.1
 dissociation-constant = 2.511886d-5
  ! K2 = dissociation constant = 1 * 10-4.6
 
 $electrolyte
 ...
 pH-value              
  = 6.4d0       
  ! 
  pH = -lg(concentration) = 6.4 ->
 [M]=[mol/l]
  (The point of zero charge for SiO2 is at pH = 2.2.)
 The Si region (1501 nm - 1541 nm) is homogeneously p-type doped with boron 
having a 
concentration of 1 * 1016 cm-3. The electrolyte region (1544 nm - 9999 nm) contains the following ions:
 
 !---------------------------------------------------------------------------!7 mM singly charged anions! The electrolyte (phosphate buffer, NaCl) contains five types of ions:
 !   1)   7 mM singly charged anions  (1-)     
<- 10 mM phosphate buffer (PBS) H2PO4-
 !   2)   3 mM doubly charged anions  (2-)     
<- 10 mM phosphate buffer (PBS) HPO42-
 !   3)  13 mM singly charged cations (1+)     
<- 10 mM phosphate buffer (PBS) Na+
 !   4)  10 mM singly charged cations (Na+)    
<- 10 mM NaCl
 !   5)  10 mM singly charged anions  (Cl-)    
<- 10 mM NaCl
 !---------------------------------------------------------------------------!
 $electrolyte-ion-content
 
 ion-number        =
1              
!
charge of the ion:ion-valency       = 
-1d0           !
 1-Input in units of:ion-concentration =  7d-3          
!
 [M] = [mol/l] = 1d-3 [mol/cm³]refers to region where 
the electrolyte has to be applied toion-region        =
1544d0  9999d0 !
3 mM doubly charged anions
 ion-number        =
2              
!
charge of the ion:ion-valency       = 
-2d0           !
 2-Input in units of:ion-concentration =  3d-3          
!
 [M] = [mol/l] = 1d-3 [mol/cm³]refers to region where 
the electrolyte has to be applied toion-region        =
1544d0  9999d0 !
13 mM singly charged cations
 ion-number        =
3              
!
charge of the ion:ion-valency       =  1d0 
          !
 1+Input in units of:ion-concentration = 13d-3          
!
 [M] = [mol/l] = 1d-3 [mol/cm³]refers to region where 
the electrolyte has to be applied toion-region        =
1544d0  9999d0 !
10 mM singly charged cations
 ion-number        =
4              
!
charge of the ion:ion-valency       = 
 1d0           !
 Na+Input in units of:ion-concentration = 10d-3          
!
 [M] = [mol/l] = 1d-3 [mol/cm³]refers to region where 
the electrolyte has to be applied toion-region        =
1544d0  9999d0 !
10 mM singly charged anions
 ion-number        =
5              
!
charge of the ion:ion-valency       = 
-1d0           !
 
Cl-Input in units of:ion-concentration = 10d-3          
!
 [M] = [mol/l] = 1d-3 [mol/cm³]refers to region where 
the electrolyte has to be applied toion-region        =
1544d0  9999d0 !
 In addition to these five types of ions, the pH value (as specified in $interface-states) 
automatically determines inside the code four further types of ions, namely the 
concentration of H3O+, OH-and the 
corresponding anions-(conjugate base: [anion-] 
= 10-pH - 10-pOH = 10-6.4 - 10-7.6 = 
3.73 x 10-7) 
and cations+ (conjugate acid; zero in this tutorial for pH = 6.4 because pH = 6.4 
< 7). For 
details, confer $electrolyte-ion-content. We have to solve the nonlinear Poisson equation over the whole device, i.e. 
including the Poisson-Boltzmann equation that governs the charge density in the 
electrolyte region.As for the boundary conditions we assume at the right boundary 
(Electrolyte/Metal) a Dirichlet boundary condition where the electrostatic 
potential phi is equal to UG where UG is the gate voltage 
determined by an electrode in the electrolyte solution and which is constant 
throughout the entire electrolyte region. In this example the applied gate 
voltage is UG = 0 V, i.e. the electrostatic potential in the 
Poisson-Boltzmann equation is fixed to 0 V. Note that the reference potential UG 
enters the Poisson-Boltzmann equation and also the equation for the site-binding 
model at the oxide/electrolyte interface. So the Dirichlet boundary condition is 
phi = 0 V. This corresponds to the fact that at the right part of the 
electrolyte,  i.e. at 'infinity' (at 9999 nm) the ion concentration is the 
'equilibrium' (default) concentration as defined in
  
$electrolyte-ion-content.At the left boundary (Metal/SiO2) we use a Neumann boundary 
condition with a zero potential gradient that corresponds to an electric field E 
= 0 V/m.
 
 
   
$poisson-boundary-conditionspoisson-cluster-number  = 1
 region-cluster-number   = 1
 boundary-condition-type = Neumann
 electric-field          
= 0d0      ! 0 [V/m]
 
 poisson-cluster-number  = 2
 region-cluster-number   = 6
 boundary-condition-type = Dirichlet
 potential               
= 0d0      ! phi = 0 [V] 
<=> UG = 0 [V]
 
 Oxide/electrolyte interface potential as a function of pH valueThe Si-SiO2 heterostructure acts as a sensor via the semiconductor-electrolyte 
interface potential that reflects sigmaadsorbed, the pH value and the 
spatial dependence of the electrostatic potential in the solution as described 
by the Poisson-Boltzmann theory. Choosing flow-scheme = 30, several 
calculations are performed while sweeping over the pH value from 0 to 14.
     pH-value              
= (value is overwritten internally in the program) The file InterfacePotentialDensity_vs_pH1D.dat gives us the 
information about the electrostatic potential at the oxide/electrolyte interface 
for different pH values. The surface potential is defined as the difference of the electrostatic 
potential at the oxide/electrolyte interface and the reference potential UG 
(Here: UG = 0 V). 
    
 Fig. 2: Calculated oxide/electrolyte interface potential as a function of the pH 
value by using the nonlinear Poisson-Boltzmann (PB) ion distribution.
 For comparison the results obtained using the linear Debye-Hückel (DH) ion 
distribution are also shown.
 As expected, in the case of zero surface potential, the Poisson-Boltzmann and 
the Debye-Hückel results are identical.
 (Electrolyte: 10 mM phosphate buffer, 10 mM NaCl)
 The slope (d phi / d pH) is a characteristic property of an 
oxide/electrolyte interface. Note that in Fig. 2 only the slope is relevant but not the 
absolute values of the potential. A linear fit between pH = 0 and pH = 9 yields 
37.7 mV/pH in agreement with experiments (P. Bergveld, A. Sibbald, Analytical 
and biomedical applications of ion-selective-field-effect-transistors, ed. 
G. Svehla, Analytical Chemistry, Vol. XXIII, Elsevier, 1988). Further below (Fig. 3) we see that the oxide/electrolyte interface charge density 
saturates at high pH values (pH = [10,...,14]). This also means that this charge 
density is then (almost) unaffected by the 
oxide/electrolyte interface potential. Thus this quantity is then determined 
purely by the Poisson-Boltzmann ion distribution in the electrolyte, i.e. by the 
concentration of OH-(and corresponding cations+) 
that are the most present ion species at high pH values.   Oxide/electrolyte interface charge density sigmaadsorbed as a 
function of pH valueFrom the file InterfacePotentialDensity_vs_pH1D.dat we also obtain 
information about the oxide/electrolyte interface sheet charge density sigmaadsorbed 
(as a function of pH value) that is determined by the amphoteric reactions at 
the oxide surface. We plot in Fig. 3 the oxide/electrolyte interface 
charge density sigmaadsorbed: 
   
 Fig. 3: Calculated variation of the 
oxide/electrolyte interface charge density sigmaadsorbed of the 
amphoteric oxide surface with the pH value of the electrolyte solution by using 
the nonlinear Poisson-Boltzmann (PB) ion distribution.
 Note that there is a range of pH values where the net surface charge density is 
close to zero.
 The calculated point of zero charge for the SiO2 surface is reached for pH = 
2.2.
 For comparison the results obtained using the linear Debye-Hückel (DH) ion 
distribution are also shown.
 
At high pH values the interface charge density 
saturates at the nominal density of surface sites because at the 
oxide/electrolyte interface all surface sites adsorbed the hydrogen ions from 
the electrolyte solution.Thus for pH values ranging from 10 to 14, the oxide/electrolyte interface 
charge density is (almost) independent of both the 
pH value and the electrostatic potential.interface-density = 5.0d14 ! [cm^-2]    
=> sigmaadsorbed = 500 * 1012 [e/cm2]
 
 
 Electrostatic potential for electrolyte gate voltage UG = 0Here we plot the electrostatic potential for a pH value of 6.4.UG = 0 V, 
i.e. we apply a zero gate voltage to the electrolyte. Note that UG is 
both the Dirichlet boundary condition for the electrostatic potential at the 
right contact as well as the reference potential that enters into the 
Poisson-Boltzmann equation (i.e. into the exponential term of the ion charge 
density).
UG is constant throughout the entire electrolyte region.
 UG =   0 V:
    poisson-cluster-number  = 2region-cluster-number   = 6
 boundary-condition-type = Dirichlet
 potential               
= 0d0      ! phi =  0 [V] 
<=> UG =  0 [V]
   
         Fig. 4: Spatial electrostatic potential distribution for pH = 6.4 in the 
electrolyte by using the nonlinear Poisson-Boltzmann (PB) ion distribution.For comparison the results obtained using the linear Debye-Hückel (DH) ion 
distribution are also shown.
 (Electrolyte: 10 mM phosphate buffer, 10 mM NaCl, UG = 0 V)
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