SOLUTION SET Chapter 12 STABLE LASER RESONATORS AND...

16
SOLUTION SET Chapter 12 STABLE LASER RESONATORS AND GAUSSIAN BEAMS "LASER FUNDAMENTALS" Second Edition By William T. Silfvast

Transcript of SOLUTION SET Chapter 12 STABLE LASER RESONATORS AND...

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SOLUTION SET

Chapter 12

STABLE LASER RESONATORS AND GAUSSIAN BEAMS

"LASER FUNDAMENTALS"

Second Edition

By William T. Silfvast

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l 11 I 2-

1. Determine the ABCD matrix for a beam translated a distance d1, focused through a thin lens of focal length / 1, and then translated a distance d2 .

lv2 ] -=. [I di_l r I 0 J l1 oi,J r r,J . {9]_ 0 I J [ Y-r1 I 0 . I L &,

l(i.] ll ol ~ f I of, J l r, .] f:11- =- 6 I J t Yr, (-~ +I) ()'

e,

I - Clf )1., d, + ol,_ ( - ~ -l-1 )

- !1, ( ~ ~' +- I)

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l If I 2-

2. A collimated beam (plane waves) arrives at a concave mirror with a focal length of : 0.15 m and is then focused by the mirror. Write out the ABCD matrix for this process. ·

i

/ ,. t

lY't\ lit s I A. iT (]\I\ + v" f> ~ \ V\ f-1 IA I t ~ ~ G' :: 0 f V' ~ ~ 0 L, I )

A 13C I) V"'-~ r V" t A f0 r T ~ ~ s /Ct..ft(fl;o, +ro ""- ,.. Vt -f-i ~ ·, t1

( v 0-~ p Ct r"' e.t I/~ I I 0 Ct x_ I ,S ') \ .$ ',

. f<_t_ f IA_ ;jt tn 0-I Wt I V' ¥" 0 V' ;

t~ ~ J ~ llr.~ ~ J ~ I 0

- ~'~ 7 l

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ell- I 2-

3. Determine whether or not the following mirror arrangements lead to stability: (a) two mirrors with radii of curvature of 1.8 m, separated by a distance of 2 m; (b) one mirror with radius of curvature of 2 m and the other with radius 3 m, sep- ·

arated by a distance of 2.3 m; (c) one mirror with radius of curvature 5 m and the other with radius 3 m, sepa­

rated by a distance of 4 m; (d) two mirrors with radius of curvature of 0.5 m, separated by a distance of 0.5 m. !

I

l w o \l\A ; ~ r .o vs R -::. I. CJ V\-\ d = 2. !IV\

F 0 v- ~ i tt- bl ) / f ~ \ 0 < ( I - 1, ) ( I - ~,_} < l

( I - 5() ( I - {) ~ ( I - 1-:e )'<-~ (_I - /, IJ / ::: l), 12 I ....

( I - ~ ) ( I - !:.:f ) -;:: ( -, Is )( t 2 j) = - 0 I D j '~ ~-ca u ill; u 11sT1;.,b'4.

c L) r<, -:. S- V\<\ ~ t. ::: °1 ""'. oil : y W\

l 1 - ?-) ( I - .:( ) ~ ( o, 2) ( - o, > ~) -= - D • tJ j] > c._ tt vi f'1 u 11 <:. T-._b~

d = (;), ~-

( / - E!J..--)( I - 01-) :: o \ o. ~ t),y

L A U I , r; (J "'t ./'1_ ,( ,.'2.. e; f 5 ;4 bi Ii ry

lA]"1-l fol ~J ~tt ll / r7

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CH- IL

4. A He-Ne laser beam of wavelength 632.8 nm operating with the TEM 00 mode and with a minimum beam waist of 0.2 mm propagates a distance of 2 in from the lo- · cation of the minimum beam waist (within the laser cavity) and is incident upon ·. a lens with focal length 50 mm. Determine the location of the focus of the bea~ : using the complex beam parameter.

\_ - -~l.

r A- r3] r, ~;i r , o] 11 =t-,J \_c O -::: Lo r J L_- '!+ 1 · L D 1

( 4 \) ({,)

A+'~\ 1.)

.. S I i'l c.P

~ {t,,)::oO

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lH- I L I

5. A Gaussian beam of wavelength 800 nm is measured to have a wavefront curvature ' of 3 m and is known to have a beam waist somewhere of 0.75 mm. At that location, :-

how far is the beam from its minimum? ~ _ \ _'t

\-=- '6 6 () V1 ~ . V\_-= I (a 1·1--" ) Y<_ ( ?:- , ) :::] ~ W{?j):: 7,) x/o 11;..

-C/ _L _ _L _ ~ )> _ \ _ /\ sooxio ~ ~-= 0.3 3- o.l/5.>; ~I - ~ l :t1) V Y\ 1f vJ '-(~) - S \ii;\ \J I 11 ( 7, ~;</O- 'I""-) V

A;! t11. k &.~ -=t::

J_ r ', f Y"b kA.. Q 2 • ~ f6) _\ -::: _O_..J-____;1:...-1 _ _

12 ) + 24x,

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CH 12-~ i '

6. How many transverse modes are lasing in a He-Cd 325-nm laser with a confocal !

cavity if the beam diameter is -measured to be 0 .1 m at a distance of 3 m from the , center of the cavity and the minimum beam waist is 50 µm? Hint: Use M 2

.

.I ,.,

r-' I t.A. v i i..t e... .,._ ~t

w~~\ - W;}·=

_, A = 3 J.. r-x 1 o """"

J r-= 3~

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C/-1-IL

i

- L/,;"' - (), ~S' j -------------,--~- ~

_ _ - 4,S"' - 0, S'S"' a . ( ( 1- Lf,S--li.) + <JtSr i-1, jJ -. Ill 3 ! - 1 '[if S?'t'T~ M ME lllffil-2 1 1i'fte7N'tf":t 'Sffii?Mj _ ' cuw

U 1 - '-I.> it,_) - &.n· ~ 3 J [l 1 - '!.> .. t.._) + o.sn~~ J]

-:: -lf.~{ I - '1::.~·) +:Yss__t- ·-~ ·~,-!,~~~~[/1 l ~~ J [ ~~-·--~--. J

'2.

~~ r~=D=;> -L/,!;,-(l-L/,)~1-) + ~,s-r)::-C

o v- - f../, s; + (J. £""') l.~2.- + (D, ~ J') ~-.:: 0

~ = 4, s - ( o,.r.r)"_ (), tt J J, ~ l Lf, > -. ----

r= vu_ CL j / ~ a_Y' i ea ,rt T

- [ tHr ( 1- 'l .. n_o. ·mJ) + '-IS ( oss-"'[o.<tsJJD ~· [(I - 4.S-[ o, 133]) ~ o. !.TfP.1~i/ iJE1 -'IS[p.'13!f) + D.!SI tJ.'iJj} 0 J = _ s--, L" s-x 10 - er a

ff W-i.(22 )

- I -1. 7 ft> + 2~ >I] j. /, ~ lf x I 0 - 7 ~ [- J, 2. - CJ, S-13 oJ [- 7. 2..+ o .. rt:sj_} :: - w2 ( 2-,) ~

- 6 ... fT' d /,~ Yxio-7 ,.

I tJ .. 2.l/ +- o, ~' J ... \N L_{ ~) - ~ (),on)":.. t (, 'fX 10- 7 7' wh.) "" 1.1'1 XIO - (.

WL{:ii.) - s w ("t'l) = /, 77x10 ~

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CH 12-.

7. A laser cavity is constructed with a pair of mirrors having a 2-rn radius of curvature, i

separated by a distance of 1.8 rn. Determine if the cavity is stable. If a 0.2-rn focal · length thin lens is mounted directly in front of the laser output mirror, where will it focus and what will be the focal spot size? The laser is an Ar+ laser operating at 514.5 nm.

r,

A :;:_ S' I 'i ) VI IM,

V\ = \

LI)= [),I

i==-1 'I"'~ r $ () I ve -1-o V" \J.,l c~.) CA_ ..... ~ R ( ~.) w 4~ ~, -:::: D, 4 l;tA.

Fov- et. s~~~r.,.,·L Lal.f1t/> .fY"f>~ (12. 'ts-) \N 7-{?;, )-;:: ~ ( . I ) -::: /, ~ ~l'-l S-XICJ-ct) (_ ( \

. .,,- \1 - ~ l n- \ I - (), o/'J -7 L.. = 2., 1'l XI 0 ~

~ ( i r< -~) - t), ~ + f, rt { l/- J, ~) = L. r< Ct:-,)= ~I + ~ ~I - Lf (, ~)

(:;ro ""- V' 6 ~fti. ~It.$ A.l-1 d_ ~"'- ftJ £.VIA

[ l ~ 'l-J r I 0 l - r I - ~·If {) I t!4 lj - L- ~

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c /.-/- / 2-

8. Determine the beam waist of a Gaussian beam of wavelength 632.8 nm after beingl translated a distance of 5 m from the location of its minimum beam waist of 100 µ,m,

transmitted into a planar piece of glass having index of refraction of 1.5 at normal incidence, and translated another 0.1 m within the glass.

--

l\ ot '-] r I o l r ' °' '1 ~ l L" ~J L 0 I

L 1

0

---

-~ :. (00 X.IO

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C/-1 IZ-

9. Design a cavity for a C0 2 laser operating at 10.6 µ.,m that would produce a beam 1

0.02 m in diameter (2w) at a distance of 2 m from the laser output mirror. State · the cavity parameters that you would use for your design. Assume the laser has a gain length of 1 m.

r '

t.( ( )"l. "l. -, - II Wo - 0 I b I wt) + /, II x I 0 -::. 0

-3 Tvvo t;6 lu ti~ ~Wt> -==- ~.17 ~,a-'-1 6"' &/.t:t, klD

Ni~r.or uu-v~~v-t: (.( { os~) = ~ [I +llf ~T} os[i + ~~&~~~o~))j

'~" -- -... , '

VVt>-:.: C(.}?XIO fQ' ( o,,s) -=- o. s; ~'° ~ l

\}Jc --:.. t:t, '1 (, )( I 0 -~ R. l (), ~} = t.7}XIO k1

For

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. cHIL 10. A TEM 00 mode He-Ne laser operating at 632.8 nm is tightly focused by a lens to 1

arrive normal to a 12-mm-thick quartz window (rJ = 1.46) at exactly the focal point .. of the lens. At that location, the 1/ e2 diameter of the beam intensity is 2 µm. What would be the beam diameter when it arrives at the other surface of the window?

> := i 3 2, ~ i-1 ~

·~ ".:' I 2- """-"""'- ':::: D,012 VA.._

d = 2 Wo -=: 2 µ ~ ~ WD -= / ,AA ~ :::.. I() - ~ M

"- 2..

Z-iz..-::: \/\._ 1r W;;, _ /,'it, 11' {!_b-~) -:::- 7. 2~XIO-tp..._ >-- u :s 2. <t' X.10-~

I - 3 ~ /, /., <R X Io ~

- - - -·----------------------:

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· · l#/L 11. A 0.1-m-long ruby laser rod is installed on earth in a symmetrical cavity with ~

external mirrors separated by 0.2 m. This laser was measured to produce a 100-km-beam diameter on the moon, a distance of 400,000 km from earth. What radius of curvature mirrors would have to be .used for the laser cavity in order to do this?

l. w

-....\ q 'l J ~ ·J..,.)x10 = w0 -1- 7,~1x10

Wo '-·

·wb L u e-V'if s ""'-~ ~ Y7 ~{ 70 r 1~-·l-r l~,r li:-r""

7,<(Jx10 3 -V>

2 ('.""""' . er :: J, I 2 x. 10 I.) XID

~ ' ( ( 11 x I 6 - ~ -::: ' /, 7 7 ~ WA

~ =- () I I IA-\.

fZ =- () , I [ I -/- ( rt [ 1. 77 x 1 o -J ') 1J ~'f't.SXlfJ-'1 (0,1) .· ..

-

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lH /2-12. An argon ion laser is operated cw at threshold on the 488 nm transition in a con- 1

focal laser cavity in which the mirrors are separated by a distance of 1 m. What would be the beam spot size and wavefront curvature at a distance of 100 m from the output mirror?

F (.) "" t)_ . {Ark- -fo wJ CA.. v I ~ ;

. =. ( M ) 11,_ - ( 1..tfJrt.'1.IO- Cj (I) ) '12 wb 1.-11 - ~ -i.11 -

:=: L , '7 7 x ltJ-'1 W\

\N-:_ Wo [1 + (;~o0J//,_

. , r f

_2 = ), ~ D x I o VV\

-- 'l.._ /DD· ~D'--~ /, /) 6 S' x I 0 - ' I

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I~, ~,) Fb V'" $'f IAA ~I V'L.C. LJJ_ I) I rz, ~

l/112..

. ~ ~ ~ WiJ :=. 2ft lJeff ( 2 V<- J"H)] -i.

-t:t // - soo; ;o [ o. <t (2 - o. ifl ,.._ ::: 7, ~ t) >< Io - q

Wo -::: 7_. /CZ. x: l ()-..., M ~ D I 7... f7 er V\I\ ~

~ .~ :. l~s, w 'l= de1+).. ( I ) rr- 1-12

~ (!?.'i;) s-00K10_, ( I ) (/ /- ~,D'-1

I -7 = /,~2-Xlt

r < w -=., 3, ~ '-{ )( t 0 - '-/

5 p o t st t:e -::: 1.. W -= _ 7, 2 ~ x to - '1 Vt~ -= D, 7 2 ~ ~ VI.\

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LH 12-13. Consider the cavity shown in the figure. Draw the equivalent lens diagram for this

cavity. What would be the values of d/f that are stable in this cavity? Use the complex beam parameter analysis along with ABCD matrices. Ford= 0.3 m and f = 0.5 m, what would be the spot size at the lens for a wavelength of 500 nm?

(, h_ &t. 1.1, tp 1'1.t_ r re Jp I e,, ~ ID o{ = DI 2.. ~ I ~ ~ lt.ttaii 1 d = t} t 3-~ __ ..;;._ __ ..:._. _____ , ___ ,,_,..._.;!!'i!l!'l~'ll'fi!*''";" ·tm . ,.. 11·e ••·Rll• --,.,m~~

d

/

d d

f

d/2 d/2

,,.A 1- "'&<.~ IA)a...1~:r a..:t- L.~ ( ~uu.~ s<:i'4-«~t.-.,t.') fV\ I J1 I IM- u. ""'-- ~ (/

Ft> v- eer; u.~ v ~.l.o--f ~ , ...- v- o ...... Ut v ~ T1 f = f<I?... :::;. i<. == 2 f

11 ~ 1~" ~ - ~) = 0 - ~ )-:o (I - 2;)

sh.~le -fo.- o < ~ - ¥/<- I

d: o, 2. ~ LJ ~ = o. <d vv._ l'<-=- 2 -f--:::. 2 (tJ,~)-:::. I M

ct-:::. I - '-~ - I - 2. ( o, i) -=- I - ~ : (), L. " -f. -. , r (),..,

( Ufvt T(v, ~ .._" )