Chapter 4.1 Applications of SHG Flashcards
(10 cards)
Auto correlator NLO involved
SHG in BBo crystal - blocked
SFG in BBO - detected (due to momemntum cons i.e. phase matching, goes stright, hence Backgroiund Free AC )
DEF
autocorrfunction
A(T) = int (-infty,infty) [I(t) I(t-T)] dt
Require time dep intensity deistruution
What is the goal of autocorrelator
Measure length of fs pulse with slow PMT elctronics
-split pulse into 2
- delay one
-focus into BBO crys
- block SHG allow SFG only at overlap
SFG relation to how much is generated vs what comes in
dA_2 proportional to E(t) * E(t-Tau) dz
incident E filed in BBO crystal is
Etot(t) = E(t) +E(t-Tau)
A2 prop E(t)E(t-Tau) L
I_(SFG) prop to I(T)I(t-T)
What does detector easure in autocorr
Slow detector meausre total Energy of pulse proportioanl to A(tau)
data process for autocorrelator
Use th measured autocorreclation function from slow detector
- fit it to autocorr of Gaussian pulse
-use FWHM to extract delta t (pulse width in time)
NB things to note in auto corr
ensure that stage movement introduces small enough delay time T such that you can map out the 35fs pulse
(1um ok prod 3fs diff)
link symmetry fo crystal fo X gen
oppositeways
Centrosymmetric - > X1 (no x2)
Noncentrosymm -> gives X2
(think of SiO breaking symm giving non zero X2)
setup for Surface SHG to analyse crystal surfaces
Fs pulse in
polariser 1 to select P of laser
sample at 45*deg to beam, rotated through phi
(crystal sample typically has X2 i.e. NOT centrosym)
output w and 2w
polariser 2 to select 2w polarisation
w1 filtered out
q2 detected plot as function of phi
results from surface SHG
Plot I (shg) as a func of phi ofr diff polarisations
#lobes show #fold symm in crystal lattice
p-p s-p, p-s s-s relative sizes tell how X dep on diff orientation of crystal