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author | prashantsinalkar | 2017-10-10 12:38:01 +0530 |
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committer | prashantsinalkar | 2017-10-10 12:38:01 +0530 |
commit | f35ea80659b6a49d1bb2ce1d7d002583f3f40947 (patch) | |
tree | eb72842d800ac1233e9d890e020eac5fd41b0b1b /284/CH8 | |
parent | 7f60ea012dd2524dae921a2a35adbf7ef21f2bb6 (diff) | |
download | Scilab-TBC-Uploads-f35ea80659b6a49d1bb2ce1d7d002583f3f40947.tar.gz Scilab-TBC-Uploads-f35ea80659b6a49d1bb2ce1d7d002583f3f40947.tar.bz2 Scilab-TBC-Uploads-f35ea80659b6a49d1bb2ce1d7d002583f3f40947.zip |
updated the code
Diffstat (limited to '284/CH8')
-rwxr-xr-x | 284/CH8/EX8.1/ex_1.sce | 26 | ||||
-rwxr-xr-x | 284/CH8/EX8.5/ex_5.sce | 45 |
2 files changed, 37 insertions, 34 deletions
diff --git a/284/CH8/EX8.1/ex_1.sce b/284/CH8/EX8.1/ex_1.sce index a564c8681..2b4144341 100755 --- a/284/CH8/EX8.1/ex_1.sce +++ b/284/CH8/EX8.1/ex_1.sce @@ -1,13 +1,15 @@ -// Chapter 8_Metal Semiconductor and Semiconductor heterojunctions
-//Caption_Shottky barrier diode
-//Ex_1//page 308
-T=300 //temperature in kelvin
-Nd=10^16 //donor impurity
-phi_m=4.55 //metal work function for tungsten
-xi=4.01 //electron affinity for silicon
-phi_bo=phi_m-xi
-phi_n=0.0259*log(2.8*10^19/Nd)
-Vbi=phi_bo-phi_n
-xn=(2*eps*Vbi/(e*Nd))^0.5 //space charge width at zero bias
-Emax=e*Nd*xn/eps //maximum electric field
+// Chapter 8_Metal Semiconductor and Semiconductor heterojunctions +//Caption_Shottky barrier diode +//Ex_1//page 308 +eps=13.1*8.85*10^-14; +e = 1.6*10^-19; +T=300 //temperature in kelvin +Nd=10^16 //donor impurity +phi_m=4.55 //metal work function for tungsten +xi=4.01 //electron affinity for silicon +phi_bo=phi_m-xi +phi_n=0.0259*log(2.8*10^19/Nd) +Vbi=phi_bo-phi_n +xn=(2*eps*Vbi/(e*Nd))^0.5 //space charge width at zero bias +Emax=e*Nd*xn/eps //maximum electric field printf('Theoritical barrier height is %f V, built-in potential barrier is %f V and maximium electric field is %f V/cm', phi_bo,phi_n,Emax)
\ No newline at end of file diff --git a/284/CH8/EX8.5/ex_5.sce b/284/CH8/EX8.5/ex_5.sce index adf372723..01a4252f9 100755 --- a/284/CH8/EX8.5/ex_5.sce +++ b/284/CH8/EX8.5/ex_5.sce @@ -1,23 +1,24 @@ -// Chapter 8_Metal Semiconductor and Semiconductor heterojunctions
-//Caption_Comparison of the schottky barrier diode and the pn junction diode
-//Ex_5/page 319
-e_phi_bn=0.67
-A=114 //effective richardson constant
-T=300
-Jst=A*T^2*exp(-e_phi_bn/0.0259)
-//if we neglect the barrier lowering effect, we have for the schottky barrier diode
-//for a pn junction
-Na=10^18
-Nd=10^16
-Dp=10
-Dn=25
-tau_po=10^-7
-tau_no=10^-7
-Lp=(Dp*tau_po)^0.5
-Ln=(Dn*tau_no)^0.5
-pno=2.25*10^4
-npo=2.25*10^2
-//the ideal reverse saturation current density of the pn junction diode can be determined as
-Js=e*Dn*npo/Ln+(e*Dp*pno/Lp)
-J=10^9*(Js+5.7*10^-13)
+// Chapter 8_Metal Semiconductor and Semiconductor heterojunctions +//Caption_Comparison of the schottky barrier diode and the pn junction diode +//Ex_5/page 319 +e = 1.6*10^-19; +e_phi_bn=0.67 +A=114 //effective richardson constant +T=300 +Jst=A*T^2*exp(-e_phi_bn/0.0259) +//if we neglect the barrier lowering effect, we have for the schottky barrier diode +//for a pn junction +Na=10^18 +Nd=10^16 +Dp=10 +Dn=25 +tau_po=10^-7 +tau_no=10^-7 +Lp=(Dp*tau_po)^0.5 +Ln=(Dn*tau_no)^0.5 +pno=2.25*10^4 +npo=2.25*10^2 +//the ideal reverse saturation current density of the pn junction diode can be determined as +Js=e*Dn*npo/Ln+(e*Dp*pno/Lp) +J=10^9*(Js+5.7*10^-13) printf('Reverse saturation current density for schottky baarier diode is %f A/cm^2 and for pn junction is %f nA/cm^2',Jst,J)
\ No newline at end of file |