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Stimulated: Dtering

The document discusses various types of Raman lasers, particularly focusing on Raman Fiber Lasers (RFLs) and their operational principles, including stimulated Raman scattering. It explains the processes involved in converting RFA into RFL, the role of fiber Bragg gratings, and the cascading effects that allow for multiple wavelength shifts. Additionally, it highlights the applications of Raman fiber lasers in fields such as laser pumping, optical fiber communication, and clinical medicine.

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23pgpe24
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0% found this document useful (0 votes)
13 views6 pages

Stimulated: Dtering

The document discusses various types of Raman lasers, particularly focusing on Raman Fiber Lasers (RFLs) and their operational principles, including stimulated Raman scattering. It explains the processes involved in converting RFA into RFL, the role of fiber Bragg gratings, and the cascading effects that allow for multiple wavelength shifts. Additionally, it highlights the applications of Raman fiber lasers in fields such as laser pumping, optical fiber communication, and clinical medicine.

Uploaded by

23pgpe24
Copyright
© © All Rights Reserved
We take content rights seriously. If you suspect this is your content, claim it here.
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Download as PDF, TXT or read online on Scribd
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l6.

3 Vaishnavi A
ypes of lasers (QspGPga4)
C. Raman Lasers

Baman Fiber Lasers (RFLs)

Raman Fiber Lasos (RF1S) tperate on the principle ct,


Stimulated Rarnan dtering (sks)
Stimulatod Rarnan Scatterfng (cRs) is a nonlinear
bptica process where a pump photon interact s with
madium, transfering eroqy to genrate a lower
energy 9ignal photon.
1t 0cc urs hen a high. frequency pump photon(hyp)
and a lower - frequency atqnal phstn (hvs) erar a
non-linear optieal mediun, uch as an optiad ber
The slgnal photon simuletes the emies ion of

another photn by stokes - Shifting the punp phot ong


energ
This result in aa signal phctun uhse
frecyuency
matches that t the input signal phcten, uhia
tha exCOSS energy from the pump photon s

trans fexd to the vibraticnal modes f te mediur


Sps fs a third- order nonunear optial procoss, which
means,its eficienty depets n tte properties cptíal matium.
Aniq ior (eray
The opicd qun of n Taman ibt
Jovetne d by the Rarnan
the ndwidthof Raman aaio i detoamined
ku th vibaationd sctun Gf
of the glas hot

tor Conveting RFA into n RFL. t req,uires

ceical focdback, achive dtraough iber Brag9


gatings (FeBac)
FBGrS defíne a iescnator that Support tscillation
at speciFic icquency chen Yeqlectana is high
Aistributed- eedback (DFB) esonat ors can ao
be used instead of FBGS

Osci llatin frequency Ys jis oer than the pup


rocyuencY Vp by a stotes ghit Ve
The stotes shi (VR) denat an the vibratim

proper tios of the host mat orial


Eibgr imple rsentatfon brought Rarman tehnoiegy to
the fore for Severa Yeans

Fiber lengths are long, hich provides higher


gain.
* Fibers have a Small Core diameter, which
Suppots strong light intera ctfon.
utin utvelnth cotot

eronission,o
pendatin nsion and timutat ed
in an 09sontl wa

Cascaded foman ber lasers


is tha th
Atuniue fatucs 6 fhrmn irteraction
shiyt te indapendent og the purnp teqyuny
Can act as a
The ist- oxder Raman. Shttod ight
dor the next - G6dor 3tokes Shipt
pump

Aesmator uxing a pair f ibor Bag gratngs ( FeG1)


lase. Thus lase
gcnerata the irst- 6rder Raman
ats as a þump i the nemt Raman sheft
Gocond- order ocilation s aeate d uuking a second
Then
Frbea Bragg Grating (tBG2).
Thi carading e$ect Continus, genenates multipl.
Tarnan hetot avelgenth.
hv
h
hvpo
hvpi

he

shis GA
Gf mutiple
multiple orders .
a) Ca scaded stokes

Phosphosiucate fiber
Aoubled clad
Y3 Siuafiber

Fe&
12 39 14g4 1239
1064 (06 4 100 50 l00%
l60%

I-pumplaser Raman wave length shifter


lase
b) Schermate of a Ramn phosphosii cate - fiber
ffber as
a double - clad Y53doped (ca
Punp sour. Pumped by a laser - dicde aNay.
tho
FB65 Yeglect Specific Ramn lase outpt

Continue nested pairs a FB s,


the Cscade can
using
until determined by the use n
utpud Couple that
diects Lght tut 0f the fiber t the desired frequenty .

Raman fibee tsew Comprising mltplk ovdes stoka


thus otter a qeatly expanded range o poscble
Shits thw
waveleng ths eund knoun as Chscaded Raman fber lasas
optial Pei o Raman ber aQu nn oa ch
hundied a9cntts
nt s uwing advanod Cngigution, uch
s see t lacis in Combipetn uth Ramn fiba ampiners
bptical powes (an be inrea sQd to the Poulirw reqime
hy empleying mixed
mixcd ae-rth (o) Rarman ampiiction
in ybt. oped fbeu.
lyHerbium
Rarnan deben lases are usefal r mny pplicatins,
1. Jaser pmping
2. cptical fibou Ceromuricatfom
3 Super Contiruum qenera tÉ m
4. Matenal Procesing
5.clinical medfcine

They partteulary suitable tor pumping Raman


ihen amptipieu în
xponso ave length ivisiom. multiplexed (DWS)
Remote pumping erbium ded fiber amnpleier s
ntvaned desiqns
Ultra - low thresheld , iqh- eficienc y, siqle
node cw Ramo fiber laseTs Fabricated în ulra - hfoh.
torotal silca microcavi ies
The most attractive feature aa RFL is that oscilatton
Ver a brad range of wnve lengths is Supported by
"pump uiavelength
Fher materla!

" Fiber Bragg gratings.

sAimulated Brfllouin Snttertng (aBS):


It Can be sed in an analsgou wny to
Cons truct Brilloun ffber lasers

bilouin frea,ue ncy shit and band width


The
are inn the vicinity bt 10 GHz and
t7or aflica fbes

Theae Vaues Ne Grdes c


des oh maqníde lower thn
Ramn Grequency ghit and
thse or the ame mateLial.
bandoiAth the

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