2.1.9 · Hardware › Band Theory & Carrier Physics
Intuition Ek-sentence wali baat
Jab carriers ek region mein bahut zyada bheed mein hain aur doosre mein bahut kam , toh unki random thermal motion se ek net drift bheed se sparse area ki taraf hoti hai — charge ka yeh net flow diffusion current kehlata hai, jo purely ek concentration gradient se drive hota hai, koi electric field ki zaroorat nahi .
Diffusion particles ki net motion hai — high concentration wale region se low concentration wale region ki taraf — jo random thermal motion se hoti hai. Inhe kheenchne ke liye koi force nahi hoti — yeh pure statistics hai.
Definition Diffusion current
Woh electric current jo tab produce hota hai jab charged carriers (electrons/holes) concentration gradient ke neeche diffuse karte hain. Yeh spatial gradient d x d n par depend karta hai, concentration ki value par nahi.
Drift se key contrast:
Drift current
Diffusion current
Cause
Electric field E
Concentration gradient d n / d x
Field chahiye?
Haan
Nahi
Proportional to
n (carrier density)
d n / d x (slope)
Intuition Random motion se
directed current kyun milta hai
Har carrier randomly move karta hai — left jaane ki utni hi probability jitni right ki. Toh net flow kyun?
Socho ek plane position x par. Left side par carriers ZYADA hain; right side par KAM hain.
Left side ke aadhe carriers randomly right ki taraf plane cross kar jaate hain.
Right side ke aadhe carriers randomly left ki taraf wander karte hain.
Kyunki left mein zyada hain, zyada rightward cross karte hain leftward se → ek net flow right ki taraf.
Koi carrier "chahta" nahi ki right jaaye. Numbers ki imbalance net flux banati hai. Isliye current ∝ slope hai, ∝ carrier count nahi.
Hum flux ko ek simple "hopping" picture se derive karte hain.
Setup: Carriers left ya right mean free path ℓ se hop karte hain har collision time τ mein. Mano v t h = ℓ / τ thermal speed hai. Ek plane x 0 par socho.
Step 1 — Count karo kitne carriers cross kar sakte hain.
Yeh step kyun? Sirf woh carriers jo plane se ek mean free path ℓ ke andar hain, apne next collision se pehle wahan pahunch sakte hain. Unme se aadhe (symmetry se) plane ki taraf ja rahe hain.
Left slab se (centered at x 0 − ℓ /2 ): rightward flux = 2 1 n ( x 0 − 2 ℓ ) v t h
Right slab se (centered at x 0 + ℓ /2 ): leftward flux = 2 1 n ( x 0 + 2 ℓ ) v t h
Step 2 — Net particle flux F (rightward positive).
F = 2 1 v t h [ n ( x 0 − 2 ℓ ) − n ( x 0 + 2 ℓ ) ]
Yeh step kyun? Net flow = (right jaana) − (left jaana).
Step 3 — x 0 ke around Taylor expand karo.
n ( x 0 ± 2 ℓ ) ≈ n ( x 0 ) ± 2 ℓ d x d n
Toh bracket ban jaata hai − ℓ d x d n , jisse milta hai
F = − 2 1 v t h ℓ d x d n ≡ − D d x d n
Yeh step kyun? Dono Taylor terms ka difference slope ko isolate karta hai, proving karta hai ki flux gradient par depend karta hai. Humne D = 2 1 v t h ℓ ko diffusion coefficient naam diya.
Step 4 — Flux ko current mein convert karo. Charge se multiply karo.
Yeh step kyun? Current density J = ( charge ) × ( particle flux ) .
Electrons (charge − q ): J n = ( − q ) F n = ( − q ) ( − D n d x d n )
J n = + q D n d x d n
Holes (charge + q ): J p = ( + q ) F p = ( + q ) ( − D p d x d p )
J p = − q D p d x d p
J n aur J p ke SIGNS kyun alag hain
Electrons aur holes dono physically high se low concentration ki taraf move karte hain. Lekin electron ka charge negative hai, isliye right ki taraf electron flux = conventional current left ki taraf — isse sign flip ho jaata hai. Isliye J n mein + aur J p mein − hai, chahe dono same − D d / d x flux use karein.
Kyun ka sketch: Equilibrium mein, diffusion current drift current ko exactly cancel karta hai (J = 0 ). q D n d x d n = − q n μ n E set karke aur n ∝ e q V / k T (Boltzmann) use karne par D / μ = k T / q force hota hai.
Worked example Example 1 — Electron diffusion current
Ek silicon sample mein electrons linearly vary karte hain n = 1 0 17 cm − 3 at x = 0 se n = 1 0 16 cm − 3 at x = 2 μ m tak. Given D n = 25 cm 2 / s . J n find karo.
Step 1 — Gradient. Kyun: linear profile ⇒ constant slope.
d x d n = 2 × 1 0 − 4 cm 1 0 16 − 1 0 17 = 2 × 1 0 − 4 − 9 × 1 0 16 = − 4.5 × 1 0 20 cm − 4
Step 2 — Formula apply karo. Kyun: J n = q D n d n / d x .
J n = ( 1.6 × 1 0 − 19 ) ( 25 ) ( − 4.5 × 1 0 20 ) = − 1800 A/cm 2
Interpretation: Electrons + x direction mein diffuse karte hain (high→low), toh conventional current − x mein hai — isliye negative sign. Magnitude 1800 A/cm 2 .
Worked example Example 2 — Einstein relation use karna
Holes ka μ p = 450 cm 2 / V⋅s at 300 K hai. D p find karo.
Step 1 — Thermal voltage. Kyun: V T = k T / q = 0.0259 V at 300 K.
Step 2 — Multiply karo. Kyun: D p = μ p V T .
D p = 450 × 0.0259 ≈ 11.7 cm 2 / s
Worked example Example 3 — Exponential profile (real diodes)
Ek n-region mein excess holes decay karte hain δ p ( x ) = δ p ( 0 ) e − x / L p ke saath, jahan L p = 5 μ m , δ p ( 0 ) = 1 0 14 cm − 3 , D p = 12 cm 2 / s . x = 0 par J p find karo.
Step 1 — Gradient. Kyun: exponential ko differentiate karo.
d x d p = − L p δ p ( 0 ) e − x / L p 0 = − 5 × 1 0 − 4 1 0 14 = − 2 × 1 0 17 cm − 4
Step 2 — Apply karo. J p = − q D p d x d p = − ( 1.6 × 1 0 − 19 ) ( 12 ) ( − 2 × 1 0 17 ) = + 0.384 A/cm 2
Positive kyun: Holes + x mein diffuse karte hain, aur holes + charge carry karte hain, toh current + x mein hai. ✓
Common mistake "Current depend karta hai kitne carriers hain par."
Kyun sahi lagta hai: Drift mein, J d r i f t = q n μ E ∝ n , toh students assume karte hain ki zyada carriers = hamesha zyada current.
Fix: Diffusion current gradient d n / d x par depend karta hai, n par nahi. Ek region dense ho sakta hai phir bhi zero diffusion current agar density uniform ho (d n / d x = 0 ).
J n vs J p par wrong sign.
Kyun sahi lagta hai: Dono carriers physically same direction mein flow karte hain (high→low), toh dono ko same current sign dene ka mann karta hai.
Fix: Flux dono ke liye − D d / d x hai. Lekin charge se multiply karo: electrons ( − q ) sign flip karta hai, holes ( + q ) rakhta hai. Result: J n = + q D n n ′ , J p = − q D p p ′ .
Common mistake "Diffusion ko electric field chahiye."
Kyun sahi lagta hai: Har current jo pehle seekhte hain woh voltage/field se drive hoti hai.
Fix: Diffusion random thermal motion + concentration imbalance se drive hota hai. Zero field se bhi bada current aa sakta hai (jaise, unbiased diode ke neutral regions ke andar).
Recall Quick self-test (hide karke answer karo)
Diffusion current kis quantity par depend karta hai? ⇒ gradient d n / d x par, n par nahi.
Fick's law mein minus sign kyun hai? ⇒ flow gradient ke neeche hota hai.
J n aur J p ke opposite signs kyun hain? ⇒ opposite carrier charge.
D aur μ ko kya link karta hai? ⇒ Einstein relation D / μ = k T / q .
Recall Feynman: 12-saal ke bachche ko explain karo
Socho ek classroom jahan saare bachche ek corner mein thuse hue hain aur baaki room khali hai. Kisi ko order nahi diya move karne ka — lekin jab bachche randomly wander karte hain, toh bheed wale corner se OUT jaane wale zyada hote hain andar wapas aane waalon se, sirf isliye kyunki corner packed hai. Dheere dheere room evenly fill ho jaata hai. Agar bachche charged badges pehne hों, toh yeh wandering ek electric current hai — diffusion current . Do jagahon ke beech crowding ka jitna zyada farq ho (jitni steep "crowdedness slope"), utna tez flow hoga.
Mnemonic Signs yaad karne ka tarika
"e-lectrons e-scape upstream" — electrons ke liye J n positive hai + q D n d n / d x ke saath; holes minus lete hain. Mnemonic: Neat plus for N, Perky minus for P.
Diffusion current kis quantity ke proportional hota hai? Concentration gradient d n / d x ke (concentration n ke nahi).
Particle flux ke liye Fick's first law batao. F = − D d x d n (flow gradient ke neeche hota hai).
Electron diffusion current density likho. J n = + q D n d x d n .
Hole diffusion current density likho. J p = − q D p d x d p .
J n aur J p ke opposite signs kyun hain jabki physical flow direction same hai?Opposite charge: electron flux times − q sign flip karta hai; hole flux times + q rakhta hai.
Diffusion ki physical origin kya hai? Random thermal motion combined with concentration imbalance; koi field required nahi.
Einstein relation batao. D / μ = k T / q = V T ≈ 25.9 mV at 300 K.
Diffusion coefficient D ki units kya hain? cm 2 / s .
Kya zero electric field mein diffusion current exist kar sakta hai? Haan — ise sirf gradient chahiye, field nahi.
Agar n uniform hai, toh diffusion current kya hai? Zero, kyunki d n / d x = 0 .
Fick's law mein minus sign physically kahan se aata hai? Net flow high se low concentration ki taraf jaata hai, yaani increasing-n direction ke opposite.
Hopping model mein D kya hai? D = 2 1 v t h ℓ (aadhi thermal speed times mean free path).
Drift current and mobility — field-driven counterpart; dono milke total J banate hain.
Einstein relation — D ko μ se k T / q ke zariye tie karta hai.
Continuity equation — diffusion + drift + recombination ko combine karta hai.
PN junction diode — minority carriers ka diffusion diode current set karta hai.
Fick's laws of diffusion — semiconductors se aage general framework.
Thermal voltage $V_T$ — Einstein relation aur diode equation mein appear hota hai.
Concentration gradient dn/dx
Imbalance in carrier numbers
Hopping picture: hop by mean free path
Taylor expansion around x0
Diffusion coefficient D = half v_th l