| 小火龙果 |
2020-05-28 16:28 |
RP Fiber Power仿真设计掺铥光纤激光器代码详解
(* y"0!7^ Demo for program"RP Fiber Power": thulium-doped fiber laser, v|r# pumped at 790 nm. Across-relaxation process allows for efficient $k3l[@;hE population of theupper laser level. UazUr=|e *) !(* *)注释语句 G?{uR6s># lLeN`{? diagram shown: 1,2,3,4,5 !指定输出图表 G`R2=bb8 ; 1: "Powersvs. Position" !分号是注释;光纤长度对功率的影响 jJY!;f ; 2:"Variation of the Pump Power" !泵浦光功率变化对信号输出功率的影响 2Yd;#i) ; 3:"Variation of the Fiber Length"!信号输出功率vs 光纤长度的变化,仿真最佳光纤长度 IY9##&c3> ; 4:"Transverse Profiles" !横向分布,横坐标为半径位置 4ze4{a^ ; 5:"Transition Cross-sections" !不同波长的跃迁横截面,横坐标波长,纵坐标为横截面 Jro%zZle 3HmJixy include"Units.inc" !读取“Units.inc”文件中内容 }#f~"-O `zRm
"G include"Tm-silicate.inc" !读取光谱数据 M)CE%/P 3/((7O[ ; Basic fiberparameters: !定义基本光纤参数 .
!;K5U L_f := 4 { fiberlength } !光纤长度 k39;7J No_z_steps := 50 {no steps along the fiber } !光纤步长,大括号{ }是注释,相当于备注
PP)-g0^@ r_co := 6 um { coreradius } !纤芯半径 m:XMF)tW N_Tm := 100e24 { Tmdoping concentration } !纤芯Tm离子掺杂浓度 (
u}tUv3 H#j Z'I ; Parameters of thechannels: !定义光信道 &ffd#2f`@ l_p := 790 nm {pump wavelength } !泵浦光波长790nm APu cA dir_p := forward {pump direction (forward or backward) } !前向泵浦 o]*#|4- P_pump_in := 5 {input pump power } !输入泵浦功率5W 6>B_ojj: w_p := 50 um {radius of pump cladding } !包层泵浦相应的半径 50um >)PcK I_p(r) := (r <=w_p) { pump intensity profile } !泵浦光强度分布 4ky@rcD 1 loss_p := 0 {parasitic losses of pump wave } !泵浦光寄生损耗为0 %CiZ>`5n# ({AqL#x`u l_s := 1940 nm {signal wavelength } !信号光波长1940nm PG/xX
H w_s := 7 um !信号光的半径 [6Gb@jG I_s(r) := exp(-2 *(r / w_s)^2) !信号光的高斯强度分布 j5>3Td. loss_s := 0 !信号光寄生损耗为0 VZArdXTP ENi@R\
p R_oc := 0.70 {output coupler reflectivity (right side) } !输出耦合反射率 7Z<ba^r} kMLWF ; Function for defining themodel: !定义模型函数,一定要有calc命令,否则函数只会被定义,但不会被执行 %7~~*_G calc Lk|%2XGO& begin 5 J9,/M0 global allow all; !声明全局变量 k9<P]% set_fiber(L_f, No_z_steps, ''); !光纤参数 g4 |s9RMD add_ring(r_co, N_Tm); &qP&=( $ def_ionsystem(); !光谱数据函数 KDX34Fr1 pump := addinputchannel(P_pump_in, l_p,'I_p', loss_p, dir_p); !泵浦光信道 gf8DhiB signal_fw := addinputchannel(0, l_s, 'I_s',loss_s, forward); !前向信号光信道 Sc zYL?w^ signal_bw := addinputchannel(0, l_s, 'I_s',loss_s, backward); !后向信号光信道 3o=K?eOdg set_R(signal_fw, 1, R_oc); !设置反射率函数 g"iLhm`L finish_fiber(); ]dKLzW:l end; zLxO\R!d 8 3wa{m: ; Display someoutputs in the Output window (on the right side): !在Output aera区域显示输出 ]D;X"2I2'b show "Outputpowers:" !输出字符串Output powers: t:G67^<3 show"pump: ", P_out(pump):d3:"W" !输出字符串pump:和计算值(格式为3个有效数字,单位W) ~)JNevLZ show"signal: ",P_out(signal_fw):d3:"W" !输出字符串signal:和计算值(格式为3个有效数字,单位W) VY5/C;0^h _8CE|<Cn 26,!HmtC ; ------------- TYQ7jt0=.- diagram 1: !输出图表1 6:(*u{ Ok=RhoZZ "Powers vs.Position" !图表名称 Wm/0Y'$r&k =hO0@w x: 0, L_f !命令x: 定义x坐标范围 U]Vu8$W "position infiber (m)", @x !x轴标签;@x 指示这些字符串沿坐标轴放置 aAr gKM f y: 0, 15 !命令y: 定义y坐标范围 n%>c4*t y2: 0, 100 !命令y2: 定义第二个y坐标范围 2,Og(_0> frame !frame改变坐标系的设置 ;oQ*gd legpos 600, 500 !图行在图表窗口中的位置(相对于左上角而言) E K)7g~ hx !平行于x方向网格 p<2A4="& hy !平行于y方向网格 pUs s_3 ^hhJ6E_W f: P(pump, x), !命令f: 定义函数图;P(pump, x)函数是计算x位置处的泵浦光功率 9w Pc03a color = red, !图形颜色 <=
xmJx-V width = 3, !width线条宽度 u2SnL$A7 "pump" !相应的文本字符串标签 w>:~Ev] f: P(signal_fw, x), !P(signal_fw ,x) 函数是计算x位置处的前向信号光功率 i 5"g?Wa2N color = blue, 5m`@ 4%)zp width = 3, .&AS-">Z "fw signal" El~x$X* f: P(signal_bw, x), !P(signal_bw ,x) 函数是计算x位置处的后向信号光功率 $Q[a^V~: color = blue, ztNm,1pnQ style = fdashed, 1Y"[Qs]"mU width = 3, t UJ m}+=> "bw signal" ][|)qQ%V Cw<bu|? f: 100 * n(x, 2), !n(x ,2) 函数是计算x位置处激活粒子数在能级2上的占比 o!`.LL% yscale = 2, !第二个y轴的缩放比例 .`OyC' color = magenta, <m"yPi3TY width = 3, m/)Wn style = fdashed, 8,BNs5 "n2 (%, right scale)" $q]:m+Fm 'J (4arN f: 100 * n(x, 3), !n(x ,3) 函数是计算x位置处激活粒子数在能级3上的占比 ;IC :]Zu yscale = 2, xr uQ=Q color = red, W_NQi width = 3, d~](S<k style = fdashed, A#gmKS<J/7 "n3 (%, right scale)" fA!uSqR$V
]o<'T.x :"9 :J ; ------------- @;iW)a_M diagram 2: !输出图表2 b]v.jgD qm-G=EX "Variation ofthe Pump Power" fLj#+h-! N4$!V}pp x: 0, 10 Iz/o|o]# "pump inputpower (W)", @x P;D)5yP092 y: 0, 10 )1%l$W y2: 0, 100 .]+oE$,! frame A2{u("^[6 hx @|:_ ? hy sgdxr!1?y legpos 150, 150 -hav/7g \$Xo5f< f: (set_P_in(pump, x);P_out(signal_fw)), !set_P_in(pump,x)改变泵浦信道功率;P_out(signal_fw)输出前向信号光 cD&53FPXC step = 5, /
AFn8=9'^ color = blue, F6*n,[5( width = 3, b
!FX]d1~k "signal output power (W, leftscale)", !相应的文本字符串标签 c <8s\2 finish set_P_in(pump, P_pump_in) S}Wj+H;
^EGe%Fq*x] f: (set_P_in(pump,x); 100 * n_av(2)), !改变泵浦信号功率对能级2上激活粒子占比的影响 D2 o,K&V yscale = 2, YGP.LR7 step = 5, -~O7.E(ok color = magenta, isaDIl;L/ width = 3, UPs*{m "population of level 2 (%, rightscale)", z; 6Tp finish set_P_in(pump, P_pump_in) XK[cbVu 8A{n9>jrb f: (set_P_in(pump,x); 100 * n_av(3)), !改变泵浦信号功率对能级3上激活粒子占比的影响 ~y.{WuUD yscale = 2, A`Vz5WB step = 5, vdFy}#X color = red, \F;V69' width = 3, V)M+dhl "population of level 3 (%, rightscale)", $2Y'[Dto\ finish set_P_in(pump, P_pump_in) (H/JB\~r RG [*:ReB9 CV% AqJN ; ------------- Ek|#P{! diagram 3: !输出图表3 LAG*H o2e aSG "Variation ofthe Fiber Length" 6/^$SWd2 zr~hGhfq x: 0.1, 5 %~`8F\Hiu "fiber length(m)", @x q_eGY&M y: 0, 10 )N`a4p "opticalpowers (W)", @y C8qA+dri frame BdcTKC hx _5'OQ'P2 hy J;|r00M $\kqh$") f: (set_L(x);P_out(signal_fw)), !改变光纤长度对信号光输出功率的影响 U4]>8L step = 20, *-~B{2b< color = blue, ". jY3<bQg width = 3, >S4klW=*I "signal output" x/*ndH qdoJIP{ ;f: (set_L(x);P_out(pump)), !改变光纤长度对泵浦信号输出功率的影响 &z[39Q{~ step = 20, color = red, width = 3,"residual pump" l:v:f@M& t(69gF\" ! set_L(L_f) {restore the original fiber length } H^cB?i OQ&?^S`8', @!z9.o; ; ------------- r|t;# diagram 4: !输出图表4 1:]iV}OFqR Jolr"F? "TransverseProfiles" p!^.;c RD_IGV I_max :=maxr(I(pump, -1, 0, 0), I(signal_fw, -1, 0, 0)) Ei!5Qya> r8\"'4B1 x: 0, 1.4 * r_co /um Lc ,te1 "radialposition (µm)", @x j+0=)Q%I= y: 0, 1.2 * I_max *cm^2 bl. y4 "intensity (W/ cm²)", @y 8&FnXhZg4 y2: 0, 1.3 * N_Tm '`g#Zo frame JBa( O-T hx =KfV;.& hy '"C$E922 q{/>hvl f: N_dop(1, x * um,0), !掺杂浓度的径向分布 $Lpt2:.(( yscale = 2, X2b<_j3 color = gray, ld58R width = 3, =C{)i@ + maxconnect = 1, MONfA;64/ "N_dop (right scale)" W=YFe<Q siveqz6h f: I(pump, -1, x *um, 0) * cm^2, !泵浦光沿光纤径向的强度分布 PM3kI\:)m color = red, s)Bl1\Q maxconnect = 1, !限制图形区域高度,修正为100%的高度 # Vz9j width = 3, ,4$ZB(\ "pump" J@RhbsZn WE""be8 f: I(signal_fw, -1,x * um, 0) * cm^2, !信号光沿光纤径向的强度分布 -V@vY42 color = blue, p9w<|ZQ]: maxconnect = 1, J6Uo+0S width = 3, dL%?k@R "signal" ^CZ!rOSv BS<5b*wG a4HUP* ; ------------- Oga/ diagram 5: !输出图表5 TJS/ O~= ?f!w:zp "TransitionCross-sections" hKP7p r 7w1~z I_max :=maxr(I(pump, -1, 0, 0), I(signal_fw, -1, 0, 0)) 3|4jS"t{f $$7Mq*a> x: 1450, 2050 qW8sJ= "wavelength(nm)", @x ` #Qlr+X y: 0, 0.6 9W3zcL8 "cross-sections(1e-24 m²)", @y I}JC ~=`j frame *?'nA{a)E hx 7b7~D +b hy tU2 8l. 5Vo8z8]t` f: s12_Tm(x * nm) /1e-24, !Tm3+吸收截面与波长的关系 qN h:;` color = red, YTH3t]
& width = 3, `I|$U)' "absorption" pR6mSfer f: s21_Tm(x * nm) /1e-24, !Tm3+发射截面与波长的关系 ! d Ns3d color = blue, QcBuUFf!c width = 3, }F3}-5![ "emission" \"!Fw)wj /VFh3n>I2
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