Electric dipole Transition moment

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Electric dipole Transition moment. Elastic and Inelastic Scattering Raman. Powerpoint Templates. Rayleigh Scattering vs Raman Scattering. Interaction between electric field of incident photon and molecule Electric field oscillating with incident frequency v i : - PowerPoint PPT Presentation

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𝜇𝑥,𝑦,𝑧𝑖𝑗 = න𝜓𝑖∗𝜇𝑥,𝑦,𝑧𝜓𝑗𝑑𝜏 ≠ 0

Electric dipole Transition moment

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Gas v1, cm-1 v2, cm-1 v3, cm-1

H216O 3657.1 1594.7 3755.9

H217O 3653.2 1591.3 3748.3

H218O 3649.7 1588.3 3741.6

HD16O 2723.7 1403.5 3707.5

D216O 2671.7 1178.4 2787.7

HT16O 2299.8 1332.5 3716.6

T216O 2237.2 995.4 2366.6

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Table 4.11: IR intensities for water. The values given are relative intensities, with the most intense assigned the value `1'. Theoretical and experimental values are from Yamaguchi et al. [161]. Frequencies are as obtained in this work.

ν Relative Intensities(cm) Present HF HF MP2 Expt.

STO-3G 6-311++G(3d,3p) 6-31+G(d)

1598 1 0.163 1 1 1

3773 0.103 1 0.159 0.110 0.0371-0.0506

3883 0.904 0.677 0.945 0.664 0.860-0.891

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Elastic and Inelastic Scattering

Raman

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Rayleigh Scatteringvs

Raman Scatteringhni

h(ni-nR)

hni

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3

2

1

0n1

Auto- IR Rayleigh Stokes Anti-Stokes NIRFluorescence Absorption Scattering Raman Scattering Fluorescence

Ener

gy

Virtual Levels

2

1

0n0

2

1

0n’1

E=hnR

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3

2

1

0S1

3

2

1

0S0

Ener

gy

Virtual Level

Rayleigh Raman (inelastic) Ressonance(elastic) Scattering Scattering Raman

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Classical Raman Physics• Interaction between electric field of incident

photon and molecule– Electric field oscillating with incident

frequency vi:

– Induces molecular electric dipole (p):

• Proportional to molecular polarizability, – Polarization results in nuclear displacement

p E

0 cos(2 )i iE E tn

0 cos 2 Rq q tn

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• For small distortions, polarizability is linearly proportional to the displacement

• Resultant dipole:Rayleigh

Scattering

Anti-Stokes RamanStokes Raman

0 00

1 cos 2 cos 22 i R i RE q t t

q n n n n

𝛼= 𝛼𝑜 + (𝛿𝛼𝛿𝑞)𝑜𝑞+ ⋯

𝜇Ԧ= 𝛼𝐸ሬԦ= 𝛼𝑜𝐸𝑜cos (2𝜋𝜈𝑖𝑡) +

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4Rh

i RA kT

S i R

I eI

nn nn n

-2000 -1000 0 1000 20000

20

40

60

80

100

Raman Shift (cm-1)

Inte

nsity

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Roto-Vibrational Raman

ΔJ = 0 ± 2Line Spacing 4B

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Ressonance Raman

Scattering effect enhanced by a factor 106

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Instrumentation

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Lasers

Ar+ ion 488.0 nm & 514.5 nmKr+ ion 530.9 nm & 647.1 nmHe:Ne 632.8 nmNd:YAG 1064 nmDiode 630 nm & 980 nm

Resolution < 6 cm-1 → Laser Linewidth < 1 cm-1

Wavelength Stabilization is a must have(most common 785 nm NIR 300 mW

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Holographic notch filter

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