solution set chapter 9 requirements for...
TRANSCRIPT
SOLUTION SET
Chapter 9
REQUIREMENTS FOR OBTAINING POPULATION INVERSIONS
"LASER FUNDAMENTALS"
Second Edition
By William T. Silfvast
C.11 q
1. Using the equations (9.8), (9.9), and (9.10) that were developed to describe changes in the populations of a three-level system, obtain expressions for the populations in the upper and lower laser levels, the inversion ratio, and the minimum pumping requirements given in (9.11), (9.12), (9.13), and (9.14).
ol /\Ii _ d.A -
ol N '< _ -c:U-
d /\./,/ -vGt
f rD~ ('1.q) '?{ (.f '~ N Ii. "=- ¥,,;CA N; (I)
f r-o ~ (Cf. 11>) lit /\l_e -:. c ~ .. /tt + YA·,i) '''" ( 2 )
(1) - '(UL N'1 --(2)
-.
1-;,i N.t
(ou; + o,,1u)N" + v . >.. / -= ¥.,,·"'" N 011 ~ I'~
(~8)
(tt' 9 J
( 1, ID)
T"~ (~IJ) o.,; tt Nt :: ¥ c.t' ( o:.u +- 'lt) /Y Lf. re;
, ~ t
, r f
( '( 1tP- + Cl';;") f\/., + ~ ( 'OJ" + ~-•e) N i.r. :: '¥.;" N I 2.l
!"114. '";, '7~- 'O,t' ~ ,_ u N (C/,/Z) r;; ( '( tt-D- +-- ~·u) + 'tfA,t ( 'ttt'"' + 'oi.o.)
f''1.e -=, ¥tte ( """' ..;.. '(.ft) ' r;.(· 'tA' !,,( ' ' ' ~~ N ,A.IA fl; I~ (¥w.+-'6~·t.t)+¥u.tCl~+t.d)
Np. ::: 0 "' ( Y"·u + a,.'J !___ . ·- {\/ ft, \ l) t;,; ( '("" ;-~.tti.) + ~.t (tit·~ t ~~)
Cll C/ 2. Referring to the example in Section 9.3 on the threshold pumping requirements for :
a ruby laser, estimate the number of pumping photons and the power required to · . pump the laser rod to the threshold value for a 6-mm-diameter, 0.1-m-long ruby laser rod doped to the concentration given in the example during a pumping cycle that lasts for the duration of the upper laser level lifetime of 3 ms. Assume that the laser is pumped by photons of wavelength 550 nm. Remember that Nofli represents the number of ground-state Cr 3+ ions pumped per cubic meter every second into the upper laser level.
=: /, t;"'/ X /D 2. 2. p/A...ofD"'-4 /':,
#- pft...,ot'o•"~-:.. (1.~1 x10'-2 ph.c!DIA<l/s.)(s ><la-)s)
-= l/. ~2. x 11J t&r p LT;;~
. J s: '-IS- x 10 ~
CH C/ 3. Beginning with the rate equations given in (9.16) and (9.17), obtain the threshold
inversion requirements for a three-level atomic laser as given in (9.21).
('f,16)
(1,/7)
(~,I~ J
f'I A r· + !'-{ t.{ 'tup u f)J_ -
V I' f'f I' + I o "" t{l-/J 0 0~ OUL + 'tuc
¥R.o ¥10
No [!~~ -r (\<~:!-i'~J i-;J
,,,. I t
Cf! ·t!f . I
4. Refer to the energy-level diagram, Figure 10-S(b), of the argon ion with the rele- . vant energy levels for the 488 .0-nm laser transition. Assuming that it operates as · a three-level laser when considering only the single-ion energy levels, what would be the maximum ratio of excitation from the ground state to the lower laser level
I
' t
1--; '-. < r !u.~ _J_ f-'ott L Au.e. t.~-
1 u -:: <.. (9 ,.) + I -:::-. G. 1.t =- {__ (!ILJ+I::: L/
bJ' Att.o : 2 3 :<' 10 f(lc +- '-/, f")< It> ~.s. +- A IJ..J_ - 7. g x I 0 7 / $
< ----
---------------------- ----- -
Cli 1 5. Given the rate equations (9.25), (9.26), (9.27), and (9.28), obtain the expressions /
for Nu, Nz, and I'oi for a four~level laser system given in (9.29), (9.30), and (9.33) . . :
cyj.t-= Y ot. Nb - ~b NL -i. ifu.1 Ni., ::. CJ
i~" "" - Y t.t.t /\I" + ¥.t" N; -= o
dAf.i ~ ":. "'~
( 9, Z-.>)
{ '1, 'J. ? )
(&/, l E?)
Frtn-- ( 'i, 2 7) '"'. ~ 1' . Ne. t)A A
S ~ ~ $ t; rfA, ti
, , '
Y .. itt ,-&.t ~ (_'1, 2,) /\{ u ~ ¥,./l.( l\f~· 'G(Ay IJ,,i No ,_,... -
¥1.-t..I;. 0 4>1;2. '6J4
Or '" tt :: (];A• /'Va
f:j_y. -N.1_ -
Yu'-
Ni. = 4"o.e 1'-lo + °(ft,.Q IV11 '::: !:E~ "!~ +- ~_, ~· /V~ 'ts't~ ~ o ~o Ytr..t
'= (¥o.1. + ~ ... ) Na ~l>
f'oA• ~0 ¥ ,,u_ ( Yot t- r;.A.) -
~~ ?l.t(;)) tr~'
-.,,.... - A/E.,o~ r ~ ::= e rllt. ){.qt)
... Aff.e~ or- 17,A· > e 'l!:f Au~
· C II 'if. 6. Determine the single-pass gain of a 0.1-m-long Nd:YAG laser rod operating at f
1.06 µ,mat room temperature. Assume the following: . 1
(a) Auz = 4 x 103 s-1, no significant collisional or phonon broadening occurs
on that transition, and there exist no radiative decay routes from level u other than to level l;
(b) the pumping level i decays primarily to the upper laser level u, and the lower laser level l decays to the ground state 0, at a rate of 1012 s-1;
(c) the lower laser level l is 0.27 eV above the ground state; (d) the pumping rate to the intermediate level i is 100 times the minimum value
given in (9.33); and (e) the doping concentration of the Nd:YAG rod is 1026 m-3 .
_ cEto_Ar A-s~u .. ~ r"- =-i.t ~ .. <-.::. I DO e ?(,,~ T _"'- 300 Jc..
r I
-~1. (-, I oo -i.,~-r!'/xto l/x. fl\ l/s o~ .:::: . e v = //, $? ~
I-, . {),( I\/ -
-- 110 ...._ 0 t.<-t_
F~ (J.3 o)
~ N 2, 97 X/O l / -:: 2.97X.IO- t> = H .. 2) 'l
Fvo~ T~ IS°'-) CJUA = 2,~ XI O k-t
~ 1• == (ti .. - N.L) i.T:f ::-(t.&/?)(to21 -2.rtx10~~2.txrr/t3.., -=- ~. l~ /tM.
r: ~,is. (.1) o.92~ r o "il.> - r L:::J - L e - e . ..... 2, "-) {')I> - 6 c;;;.. - •\ 4:..- 0 v ~ t ~ -
L-fl 1 7. Beginning with the differential rate equations (9 .35) and (9 .36), solve for the ex
pressions for Nu and Nz as a function of time as given in (9.37) and (9.38).
,. ,. I
~'f :: No (ID'< - N"' Aw
d..:: ::: N D 1-;.e + /\/ ~ A l{.Q_ (q, 3ft;)
A-ss UiMe No = tAP---rr~-:t (o_ ~et. sc~-bte o_t;.t;v .• A·•--r;r;~) fr.- , 1 ( -A411 .:r )
~ a...ss~ ec 50 lt..(_tt/f'\ fv"- /\II.{_~ lvtt::::.C.1 t-e
( r;;, ) A r - ( ,_ e-A"'~ :r\ -n- +- I tu. ) I bt.t
c, :.. ~!7t>N-1
- - -----
{_JI q. 8. Referring to the energy-level diagram of the lead vapor laser of Problem 8 in Chap- \
I
ter 4, graph the time dependence of the population inversion (in real time) of the : · I 3Pf ---7-
1 D2 722.9-nm laser transition, assuming that (a) the pumping flux to the upper laser level is twice that to the lower laser level and (b) the pumping is applied at a constant rate beginning at t = 0. Assume that radiation trapping prevents any decay to the three levels (3P2 , 3Pi, 3P0 ) below the lower laser level, and assume there is essentially no decay to the higher-lying 1S0 level as shown in the figure.
, : A 1 rr· .;- Ac_3,,,,0 _..., 'i)J-:: lf. "Ix tb s Is
~ 1'-:. -::: f I - = /,I 2. X Io -lt S II\, A "3 P.f) <Z'· 1 Xld'l> ,
- ;r/,, x 10-··il s - e ''·
- { - e-' -N ... __ ( ') - 0,423> ~ /, i;- - I - e-
1. 0
0
L_fl ~
9. At what electron density would radiation trapping begin to slow down the decay of I the lower laser level of the He-Cd laser transition at 441.6 nm? Assume a plasma tube radius of 1 mm. Assume that the gas temperature is 350°C and that half of the ions in the discharge are Cd+ ions while the other half are He+ ions. Assume also that there are no other ions in the discharge and that charge neutrality exists: the total electron charge of the free electrons that provide the discharge current equals the total ion charge in the discharge. Use the energy-level diagram and the associated coefficients of Figure 9-7 for the relevant Cd+ energy levels. Hint: The Cd+ ion ground state is the state that causes radiation trapping on the decay of the lower laser level, and its population accounts for half of the free electrons that make up the electron density in the discharge (the other half are He+ ions).
f(q_p(( cvfi°'
, , (
IVtLpp1~ bkw,~~ st~w.;f1i."'J w ~ CJ~ Nti b -=- I, '-I~ (9, '17)
CjR ":: 2{!f J t I::: Lf
1" ~ 2 (~J ti ;:_ 2-
T= 3~D+2 7 3 ::,23~
b:::.lD->VV\
Cll-1 10. At what population density of the argon ion ground state would radiation trapping
begin to reduce the population inversion for the laser transition of Problem 4? Assume a discharge tube diameter of 2 mm and a gas temperature of 600 K.
("-{ 0 :::
~ it .e -:-- '-I !6 ~. o ""- vv....
"'R.o -= 7'2. 3 vi~ lo :::. I lM \,/IA.
(Yf N ::. . '-( D
(:::- fa 60 (<.
f.e = 2~)+ I :: lf
1 D := "2 ( 3/i ) + I :; L(
/,'-I~ -
II(~,)
I{- w~ \~L l~~ /\l.t ~
,
r '
, r •
'(l..l.e. ~ Aut_::: 2. '7 rx /()I~ 'I H
'610 ~ l+.to-= 2: A.1,,
4./-j. Sott:.e f()r & ~ lflff'e.
t..t .A.-1,,,.Jro~s td~.._,e;ueJ
-: '5'1 L/.'l'XIO<i-:: 2.~'"/XI0 11
N.e = I. s x1a~r1.1~x1b" '-J ;;._, 1'-/'>( J{) II
I .,.. f '[ 7 u 'l." It I. 2.SXJ0
1q7 -=.. , S'I XI i /. ~ --, XI D - e _j
:::: I "'' 3 I VV\
Cl-/ 1 11. For the H-like n = 3 --+ n = 2 transition of the B4+ ion, what is the maximum ·
electron density at which a population inversion could occur for an electron and ion temperature of 300 eV? What would the gain be on that transition under those conditions, assuming that the pumping flux to the lower laser levels (other than radiative decay from the n = 3 level) is negligible? Assume that the population in the upper laser level is io-5ne. Note that the transition probabilities for H-like ions scale as Z 4 compared to hydrogen and that A 32 = 4.4 x 107 s-1 for hydrogen.
n~)( = o, I 3> {T; Te (I<)
'A~,, '>- ( t.-\ll*'-) ~-= ~ ~ p/!+
Vl~ e :::
~ ti
~:,--,,3
l S")'---
(), /J {?..'f'i'XIO" -;::. /, ')'f)(IO "l'l/.M.)
(2 ~,2~ X ID-~ ) 3
12. For a discharge -pumped gas laser medium, assume that the electron pumping flux is twice as great to the upper laser level as to the lower laser level. Also assume ·!
that the decay rate from the lower laser level is twice as great as that from the upper · laser level. The decay from the upper laser level goes only to the lower laser level and there is no other source of excitation to either the upper or lower laser levels than those just described. What is the ratio of Nu to Nz under these conditions? What would the value of the trapping factor Fzo (see eqn. 9.45) have to be in order to equalize the populations of the levels? Assume that the statistical weights of both laser levels are the same.
c ti.) 1)1 --d tA_
r I
/\I 4 t!".J CVR - -l'\/.e ;u.
bJ ~~:::. tL<
-_..,
(' + '~){- ) r:)IA
~p _J -Gu - '-
;
r I f=jc-=: c I ) l It :;- ) -
"L....
----- ---------
A,o Avi
A1.o :: 2.. A t.<..t
2 - t,3'3 (. ~