solution set chapter 13 special laser cavities ......chapter 13 special laser cavities and cavity...

11
SOLUTION SET Chapter 13 SPECIAL LASER CAVITIES AND CAVITY EFFECTS "LASER FUNDAMENTALS" Second Edition By William T. Silfvast

Upload: others

Post on 07-Mar-2021

3 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: SOLUTION SET Chapter 13 SPECIAL LASER CAVITIES ......Chapter 13 SPECIAL LASER CAVITIES AND CAVITY EFFECTS "LASER FUNDAMENTALS" Second Edition By William T. Silfvast CH/} 1. In designing

SOLUTION SET

Chapter 13

SPECIAL LASER CAVITIES AND CAVITY EFFECTS

"LASER FUNDAMENTALS"

Second Edition

By William T. Silfvast

Page 2: SOLUTION SET Chapter 13 SPECIAL LASER CAVITIES ......Chapter 13 SPECIAL LASER CAVITIES AND CAVITY EFFECTS "LASER FUNDAMENTALS" Second Edition By William T. Silfvast CH/} 1. In designing

CH/} 1. In designing an unstable resonator for a 248-nm KrF excimer laser, for practical

considerations it is desirable to have a relatively long gain medium such that the separation between mirrors is 0.5 m. For a magnification factor of 5, what would be the radii of curvature of both the output mirror and the rear mirror? If the laser cavity were to be designed for minimum diffraction losses, what would be the di­ameter of the output mirror?

0 2. ol '" - R.. ;:: r o

s- Rb - R.o = 2 ol

r<,, -::: ~ ::: i._ ""'- (). 2. > """'

r< ,.- ::: I ~ _/.. {). 2. '5 ~· = I I 2 S"' """"

a.• = ( os) A J L ?;f) = (o,s )(2 'H x10- ~~.s) V a. ::: ~r '6 X I b - '1 ::: {). '6 g ~ vt.-\

Page 3: SOLUTION SET Chapter 13 SPECIAL LASER CAVITIES ......Chapter 13 SPECIAL LASER CAVITIES AND CAVITY EFFECTS "LASER FUNDAMENTALS" Second Edition By William T. Silfvast CH/} 1. In designing

L/1 13

2. Beginning with (13.4), the constraint for a positive-branch confocal resonator that . Rr - R 0 = 2d, obtain (13.10) and (13.11).

bu.:f ~t> 'h.A-~ ~;~/,l,rf Lu~vetlu~ Sc ~ r-ep 1,_,u... Rb w i 71.. - R.0 7J; o b r;,,"'

r<.r + R.0 = 2 d. o ~ & + ~ :::: e;/ "2.. "2..

I - !:f 12.z...

d - l - t>l t - -'t<r

cq -:: ..!.. (I~ ~\ q-' ""2. ~,. J

Page 4: SOLUTION SET Chapter 13 SPECIAL LASER CAVITIES ......Chapter 13 SPECIAL LASER CAVITIES AND CAVITY EFFECTS "LASER FUNDAMENTALS" Second Edition By William T. Silfvast CH/} 1. In designing

CH 13 3. A 0.1-m-long Nd:YAG laser rod is installed in a 0.4-m-long laser cavity of a .

Q-switched laser. Determine the approximate value for ts and show that it is sig­nificantly shorter than r u, the upper laser level lifetime.

f ~ l'Vt l ~ I L_

w k tM. L is ~ elf e.cT/ Vt' ;a1 .... '-t /.tJ..1'1t' fit

~ M ;- I "2 I 1- /'-I 2--I I -1 I'" L /() 1-'k

_, 0,1~

~ ' . .._

e:l U. lf't:t...11 (.f"1 ;t; ~ M \ Ii'\. I Id~. lA. 11\,\. 1-41 (;o\_ ~ ""' }:iea.,~ {b ~4.. e,,l_ rs ea IS :

.;f$ = ~ [ V'tc. C d-L)+- "h. L "] ~ c.

ti.[1 · ( (),'f- a.1)+ 1.~1(".1)l T .... . . ' ' . .. -• .. ,. M '>'M!e!Hf~

1 ><10'3

=

Page 5: SOLUTION SET Chapter 13 SPECIAL LASER CAVITIES ......Chapter 13 SPECIAL LASER CAVITIES AND CAVITY EFFECTS "LASER FUNDAMENTALS" Second Edition By William T. Silfvast CH/} 1. In designing

C/-11.3 4. A 0 .1-m-long ruby laser rod has the mirrors coated on the ends of the rod. The

output mirror has a reflectivity of 90% and the rear mirror a reflectivity of 99.9%. If there is no excited state absorption (i.e., a = 0) in the laser, what would be the fractional loss per pass in the laser cavity, and what would be the decay time of the cavity?

~o \M. ( : ~, 38) I a )'12.. L F :: K L - fa l~', f( 'l..

hJ O(_ .::;.. 0

,', Lr--= -A (~,Je"l) 1l1...: -{A(R, R~) ~ _ { ~ [< ll. 'l"i41){o.9~ -=. + o, as-J

f~ (~,j<"f)

~"!! V\d -L LF

=:'II VIS

/, 7, (() ,I )

3 X IO~ tJ~ OS°']

Page 6: SOLUTION SET Chapter 13 SPECIAL LASER CAVITIES ......Chapter 13 SPECIAL LASER CAVITIES AND CAVITY EFFECTS "LASER FUNDAMENTALS" Second Edition By William T. Silfvast CH/} 1. In designing

Cl-l-13

5. What would be the maximum Q-switched power output from the ruby laser given . in Problem 4 if the mode occupies a diameter of 2 mm within the rod? Assume that the laser gain is 100 times the threshold value. Hint: Determine 6Nuz from the equations of Section 13.10.

Mb-=- IDD .AN V = /DD .t:.N rrd. 'L ' LJ

::. I D D rr d_ '- I ~ /_I ) ~ a;, \ft t 1<. '-

7: I OD fr (_1 x.wif I o..J I J ~ 2, ~x / o -L '-I ,..-L ( o. '1 11'?) { a. tf) j

-:::. "'' ~ ~ X. ID 1 f

Mf) J,. v ----":..

Page 7: SOLUTION SET Chapter 13 SPECIAL LASER CAVITIES ......Chapter 13 SPECIAL LASER CAVITIES AND CAVITY EFFECTS "LASER FUNDAMENTALS" Second Edition By William T. Silfvast CH/} 1. In designing

CH/3

6. Obtain (13.23), the expression for photon density, from (13.22). Obtain the value . of M where¢ is a maximum.

-&f M

d If/

~tr~~ f.P-= ~ ~ M - tf .J.. l..

= -4_ ( M rk. J~ 1'1 - M) + c.

w ~ LO~ lPu > /''1 :- IYfo

~ ', lP o '::. -i: ( M 1°1\ .,t..,, 1'10 - t14) + c.

o.,.. (_ ::: ~o - { ( 1"11"1\ ~Mo -MA)

, ", ~ - f.Pb ~ ~ [ l"lri- A ~ - (M - M,)]

~-A ': ('1.!it J_ - j_ ) "':. 0 ~ I "'I "'2- /V{ 2.

IV/a. - I = D Olr M = M~

'""'

Page 8: SOLUTION SET Chapter 13 SPECIAL LASER CAVITIES ......Chapter 13 SPECIAL LASER CAVITIES AND CAVITY EFFECTS "LASER FUNDAMENTALS" Second Edition By William T. Silfvast CH/} 1. In designing

C.1-f I 3

7. What would be the minimum pulse duration of a mode-locked alexandrite laser? . If the separation between mirrors is 2 m and the alexandrite laser rod is 0.1 m long, what would be the separation bet~een mode-locked pulses?

e:. Ap= 1 -= :::: ~ . t:[-;;-x101'ts

61/FW lttrt 2#l. >e IO Jj/ s

4 ;t !.fJj' -.. _!_ -= 2 [ V\<- ( d-L)+ V\1. L]-:::. ~1) c.

2 [1 {d ·l)-1- Yl~ L] WiJ2111i · w W 2 i'rU; 'N:ln!M·~

c..

- 2 u2 ..... _ o.,,.._1+ 1.?"i t"·'""'TI ~~t~r~~~

~ 'K I 0

f, ~ ~ X I o - g S :::: t 5, g' vt .$ --

Page 9: SOLUTION SET Chapter 13 SPECIAL LASER CAVITIES ......Chapter 13 SPECIAL LASER CAVITIES AND CAVITY EFFECTS "LASER FUNDAMENTALS" Second Edition By William T. Silfvast CH/} 1. In designing

!.H 13

8. For a gallium arsenide distributed feedback laser in which only the index of re­fraction is modulated, what would be the necessary index modulation in order for the laser to operate with this type of resonator? Assume that the laser cavity is 0.5 mm in length. What would be the bandwidth of the laser output?

fo " '" ~ .....e tLJ...,TI IJ"k. i j1...&... ~ ~J. ; s L-:: D, IJ 4 a S-w...

~-:: ~?O ~IN\.

Y\::: s. '-/ 2 C?i L-

& ~ e ,

~ & = IJ ()() o

, ,. ,

- >.o ~ l1D" o '1., - I), OIJOS- - ff {t ooa)"i

- 't?b x.10-" ).M.lo ~-- S°'X lttt.f Tr ( 11'f)b)'h ..

-::. $,. S-~ X I 0 -~

~'). (J,~ )<IOS)( <6?~1({0- <t..,.)

--- II 3. /(;) ~I 0 M-\

- - - - - - -----------

Page 10: SOLUTION SET Chapter 13 SPECIAL LASER CAVITIES ......Chapter 13 SPECIAL LASER CAVITIES AND CAVITY EFFECTS "LASER FUNDAMENTALS" Second Edition By William T. Silfvast CH/} 1. In designing

CHIJ

9. A hypothetical gas laser operates at 200 nm in a cavity with mirrors separated b , 2 m and is dominated by Doppler broadening with a Doppler width (FWHM ) of 4 x 109 Hz. The gain for a single pass through the amplifier is 12o/o, and each mir­ror has a reflectivity of 98%, a transmission of 1 %, and a scattering loss of 1 %. There is also a scattering loss of 0.5% at each Brewster window. If this laser ere mode-locked, what would be the maximum number of modes that could contribute to producing mode-locked pulses, and what would be the minimum pulse width of each pulse? What would be the separation between pulses?

.... ' c,. v::: {t!,)~ A ,;o =- (), 7H A Ye "t

~ Or 71J7 ( '-/X JO'( ff.;.) ':: 2, ~ "J... X /~ /-f.i;..

,

_/\ -iP t.LW> ::: ..s.. -::. - '3 x I 0 ~ ':. 7' !:>-X IC) 7 H-e-

~ -- f 7-d L.. { "l. j,6o\, l

.# 14M>~ = ~ ~ .tx IQ.: +-I ::- 1 ~ ' + I -;= 3 ~ /.U.-/J~ 7. S"' 'XII)

Page 11: SOLUTION SET Chapter 13 SPECIAL LASER CAVITIES ......Chapter 13 SPECIAL LASER CAVITIES AND CAVITY EFFECTS "LASER FUNDAMENTALS" Second Edition By William T. Silfvast CH/} 1. In designing

c 10. You have the opportunity to observe a three-mirror laser cavity (such as that o .

in Figure 13-31) in which the laser is producing mode-locked pulses at inte · -of 12.0 ns. The focal length of both M 1 and M 2 is 0.1 m. What is the di t e between M 2 and M 3? If the mode-locked pulses have a width of 133 f and J·o know that the laser is mode-locked over the FWHM of the laser gain medium, what would you suspect is the gain medium?

, r I

+-=- o, I VtA.

2 of ~ d_-: I, ge:, Vt-\ c

J., $ r~~ 1; /V[ 1- ;r;: 1a i "l C£-,/ ( 15 . Or IM

1Ct. i vt Ce./ ( fl> 1'41 IS 2 -f =: f< :. (), 2 /AA.

~ '

r ',. dt S fa.1t_c.p frip....,_ /Y/L t M;, /J I, 81 - tJ,f - IJ, 2 :;. /, )~ kA...

p~ ht1.. b 17 IV d / G-/et.e;. s &f 7,,s-- ~ /'() IL H rt: