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Basic Current Mirrors and Single‐

Basic Current Mirrors and Single‐

Stage Amplifiers g p

Hossein Shamsi Hossein Shamsi

١

(2)

Simple Current Mirror

ds out

W r r

⎜ ⎞

=

2

in

out

I

W L W

I ⎛ ⎞

⎜ ⎞

=

2 in

out

L W ⎟

⎜ ⎞

1

eff

out

V

V ≥

٢

(3)

Common‐Source Amplifier

٣

(4)

Source‐Follower or Common‐Drain Amplifier

gs1 denotes the body effect. (gs1 =gmb1) gs1 denotes the body effect. (gs1 gmb1)

۴

(5)

Common‐Gate Amplifier

2 ds

L

r

R =

۵

(6)

Common‐Gate Amplifier

۶

(7)

Source‐Degenerated Current Mirrors

in

out

I

L I W L

if W ⎟ ⇒ =

⎜ ⎞

= ⎛

⎟ ⎠

⎜ ⎞

2

1

L

L ⎠ ⎝ ⎠

1 2

eff out

s

out

R I V

V ≥ +

٧

(8)

High‐Output‐Impedance Current Mirrors

Cascode Current Mirror Wilson Current Mirror

٨

(9)

Cascode Current Mirror

L I W

I

2

⎟ ⎠

⎜ ⎞

=

in

out

I

L I W

1

⎟ ⎠

⎜ ⎞

= ⎛

٩

(10)

Wilson Current Mirror

L W ⎟

⎜ ⎞

in

out

I

L W

I L

2

⎟ ⎠

⎜ ⎞

= ⎝

L ⎠

1

١٠

(11)

CASCODE Gain Stage

telescopic-cascode amplifier folded-cascode amplifier

١١

(12)

Telescopic‐Cascode Amplifier

R

R ||

out m

V

L d

out

R g

A

R r

R

×

=

1 2

||

The folded-cascode amplifier is analyzed similarly.

١٢

(13)

Differential Pair Differential Pair

After a few manipulation, it

i th t

r r

r ≅

is proven that:

2 4 ds ds

out

r r

r ≅

Besides, we have:

i

g v

g v i

i

sc

≅ 2 i

s

2 g

m

g

m

v

i

i

1 1 1

2 2

2 = =

So the voltage-gain is obtained:

So, the voltage gain is obtained:

out m

V

g r

A =

(14)

Frequency Response

Common‐Source Amplifier Common Source Amplifier

١۴

(15)

Frequency Response Common‐Source Amplifier p

Assuming that poles are real numbers and ωp1<< ωp2, we have:

١۵

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Frequency Response Common‐Source Amplifier p

If the poles are complex conjugate, we will write the above transfer function as follows:

( ) g R

A 0 = −

m1 2

b

= 1 ω

0

a Q = b

Si il l l th C D d C G lifi

١۶

Similarly, we can analyze the C.D and C.G amplifiers.

(17)

Frequency Response CASCODE Amplifier p

p

R C R C

1 1

1

≅ ≅

ω

2

g

m

ω ≅

L out d

out

p1

R C

2

R C

2 2

s

p

≅ C

ω

١٧

Referensi

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