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Phase Matching Alex Filin Everything you always wanted to know about it but were afraid to ask

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Page 1: Alex Filin - Temple University · Alex Filin Everything you always wanted to know about it but were afraid to ask. Outline • Introduction: Origin of Optical Nonlinearity • Phase

Phase MatchingAlex Filin

Everything you always wanted to know about itbut were afraid to ask

Page 2: Alex Filin - Temple University · Alex Filin Everything you always wanted to know about it but were afraid to ask. Outline • Introduction: Origin of Optical Nonlinearity • Phase

Outline

• Introduction: Origin of Optical Nonlinearity

• Phase Matching in SHG • Phase Matching in CARS• Conclusion

Page 3: Alex Filin - Temple University · Alex Filin Everything you always wanted to know about it but were afraid to ask. Outline • Introduction: Origin of Optical Nonlinearity • Phase

Origin of optical nonlinearity:mechanical analog

Linear conditions

Force:kxxF )(

Potential:2

21)( kxxU

Nonlinear conditions

Force:3)( xkxxF

Potential:42

41

21)( xkxxU

Page 4: Alex Filin - Temple University · Alex Filin Everything you always wanted to know about it but were afraid to ask. Outline • Introduction: Origin of Optical Nonlinearity • Phase

Origin of optical nonlinearity:Polarization

Page 5: Alex Filin - Temple University · Alex Filin Everything you always wanted to know about it but were afraid to ask. Outline • Introduction: Origin of Optical Nonlinearity • Phase

Origin of optical nonlinearity

...)( 3)3(2)2()1(0 EEEP

Linear conditions Nonlinear conditions

EP 0Where P is polarizationo is free-space permittivity is susceptibilityE is electric field

Where(i) is nonlinear susceptibilityof ith order

Page 6: Alex Filin - Temple University · Alex Filin Everything you always wanted to know about it but were afraid to ask. Outline • Introduction: Origin of Optical Nonlinearity • Phase

Origin of optical nonlinearity

...)( 3)3(2)2()1(0 EEEP

• All mixing phenomena,involving generation of sum and differencefrequencies (SHG, parametric amplification)

• Pockels’ effect• Optical rectification

(2) vanishes in media with inversion symmetry

• Third Harmonic Generation • Kerr effect• All types of FWM phenomena,

including CARS

Page 7: Alex Filin - Temple University · Alex Filin Everything you always wanted to know about it but were afraid to ask. Outline • Introduction: Origin of Optical Nonlinearity • Phase

Second Harmonic GenerationWhy does phase mismatching happen?

E(z)

E(z)

E(z)

z

z

z

t1

t2

t3

Page 8: Alex Filin - Temple University · Alex Filin Everything you always wanted to know about it but were afraid to ask. Outline • Introduction: Origin of Optical Nonlinearity • Phase

Second Harmonic Generation

)(sin

)(cos

),(1

2

2

2

2

2

eoe nnn

In an uniaxial crystal

where ne and no are indexes of refraction for extraordinary and ordinary rays, respectively, is angle between k and optic axis of the crystal Phase matching conditions: = and Or n2 = n , but n = k/2 and n2 = (/2)k/2

So, 2k= k, or

)(),( oe nn

k = k(2) - 2k() => 0

Page 9: Alex Filin - Temple University · Alex Filin Everything you always wanted to know about it but were afraid to ask. Outline • Introduction: Origin of Optical Nonlinearity • Phase

Second Harmonic Generation

kkzezE kzi

)2/sin(),( 2/2

One can show, that electric field

And Poynting vector

2

2

2 )()2/(sin),(

kkzzS

2)2/sin(lim

0

zkkz

k

Because

=>

In ideal case (k = 0)

22

2

),(

),(

zzS

zzE

Page 10: Alex Filin - Temple University · Alex Filin Everything you always wanted to know about it but were afraid to ask. Outline • Introduction: Origin of Optical Nonlinearity • Phase

Second Harmonic GenerationIn real case k never is equal to 0,So, SHG power oscillates with z

Finally, phase matching for SHG requires 2 conditions:

a) Correct angle between k and crystal axis to reach

k = k(2) - 2k() => 0

n2 = nor

b) Correct crystal length to reach maximum SHG power

Page 11: Alex Filin - Temple University · Alex Filin Everything you always wanted to know about it but were afraid to ask. Outline • Introduction: Origin of Optical Nonlinearity • Phase

Coherent Anti-Stokes Raman Spectroscopy (CARS)

P

P

S

CARS

• q1 and q2 correspond to P• q3 corresponds to S•P –S = Raman is the Raman shift (Raman active vibrational mode)

Raman

Laser P

Laser S

2P-S

q1

q2

q3

Sample

2P = S + CARS

Page 12: Alex Filin - Temple University · Alex Filin Everything you always wanted to know about it but were afraid to ask. Outline • Introduction: Origin of Optical Nonlinearity • Phase

Coherent Anti-Stokes Raman Spectroscopy (CARS)

2

2222)3(

420

2

2

)2()2(sin

LkLkLII

cnnnI SP

CARSSP

CARSCARS

Intensity:

After Maker and Terhune (1989)

Where:

in i

iIis the refractive index at frequency

is the intensity of i-th signal

L is the interaction length

CARSSP kkkk

2kCARS

kS

kP1 kP2

Phase matching for BOXCARS

Page 13: Alex Filin - Temple University · Alex Filin Everything you always wanted to know about it but were afraid to ask. Outline • Introduction: Origin of Optical Nonlinearity • Phase

kCARSkS

kP1 kP2

Geometry of laser beams for BOXCARS Phase matching for BOXCARS

Principles of BOXCARS Method

Lens 2

CARSPump

Stokes

Mask Lens 1

PS

f

h

d

|kP1| |kS| |kCARS|2 = +

2Pump=Stokes + CARS

12sinsin Stokes

PumpPS

For h << f

12)( Stokes

PumpStokes dh

or

Page 14: Alex Filin - Temple University · Alex Filin Everything you always wanted to know about it but were afraid to ask. Outline • Introduction: Origin of Optical Nonlinearity • Phase

Phase Matching in fs-BOXCARS

12)( S

PS dh

)( 11 Sh

)( 22 Sh

h

I

h

r0

r0

f

f

2

0

20

0 2))()((exp)()(

rhhII

Page 15: Alex Filin - Temple University · Alex Filin Everything you always wanted to know about it but were afraid to ask. Outline • Introduction: Origin of Optical Nonlinearity • Phase

fs-CARS: Theory

222

21 1 12 2 2

1

2

21 Erf,

C S C

CARS C S

iS CI e B Aie

2 ;S P S R PC S

21 ;2

S SP

P P

FWHMFWHM

2

4ln 2P

P

FWHM

Where: normalized CARS frequency and normalized Stokes detuning

Page 16: Alex Filin - Temple University · Alex Filin Everything you always wanted to know about it but were afraid to ask. Outline • Introduction: Origin of Optical Nonlinearity • Phase

Phase Matching in fs-BOXCARS

2

222

)2()2(sin

LkLkLIAII SPCARS

ps-CARS:

fs-BOXCARS:

fr

dr

hrGII

S

S

C

CSCCARS

REALCARS

000 ,,,,),(

2

0

22

0

2

00

32exp,,,

rh

rd

dr

hrG

S

S

C

C

S

S

C

C

So far:

Page 17: Alex Filin - Temple University · Alex Filin Everything you always wanted to know about it but were afraid to ask. Outline • Introduction: Origin of Optical Nonlinearity • Phase

1.60 1.70 1.801.60

1.70 1.80 80 40 0 -40-80

Stokes Detuning, meVCARS Photon Energy, meV

CARS Photon Energy, meV80 40 0 -40

-80

Stokes Detuning, meV

Phase Matching in fs-BOXCARSOur results

Without G-correction With G-correction

Page 18: Alex Filin - Temple University · Alex Filin Everything you always wanted to know about it but were afraid to ask. Outline • Introduction: Origin of Optical Nonlinearity • Phase

1000 18001400 2200Wavenumber, cm-1

0

0.5

1In

tens

ity, a

rb.u

nits

- experiment- no correc. - with correc.

Phase Matching in fs-BOXCARSComparison theory and experiment

Page 19: Alex Filin - Temple University · Alex Filin Everything you always wanted to know about it but were afraid to ask. Outline • Introduction: Origin of Optical Nonlinearity • Phase

Conclusion

• Every nonlinear optical phenomenon requires it’s own unique approach to understand the phase matching conditions

• Understanding of phase matching is crucially important to run a nonlinear optical experiment correctly and for interpretation of it’s results.