R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies...

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R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY OF SURFACE ENHANCED RAMAN SCATTERING OF ALIZARIN AND CRYSTAL VIOLET DYES

Transcript of R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies...

Page 1: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

R. Gopal & R.K. Swarnkar

Laser Spectroscopy & Nanomaterials Lab.Centre of Advanced Studies

Department of Physics

University of Allahabad, INDIA

STUDY OF SURFACE ENHANCED RAMAN SCATTERING OF ALIZARIN AND CRYSTAL

VIOLET DYES

Page 2: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

Out line

• Objective

• Introduction

• Experimental technique

• Result & Discussion

• Conclusion

Page 3: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

Objective

Study of SERS of Alizarin dye on Ag colloidal NPs synthesized by PLA.

Study of SERS of Crystal Violet on Cu2O @ Cu NPs synthesized by PLA.

Study the effect of halide ions on SERS of these dyes.

Page 4: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

Surface enhanced Raman scattering (SERS) revolutionalised the Raman spectroscopy in the last decade.

SERS is based on the marked enhancement of Raman signals of certain molecules when they are placed in the proximity of certain nano-structured metallic surfaces.

Two types of mechanisms (Electromagnetic and Chemical Enhancement) are currently used to explain the SERS phenomenon.

PLA in liquid medium is an excellent technique to synthesize colloidal NPs with desired shape and size and surface free from chemical contamination, which is essential requirement for surface application.

Introduction

Page 5: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

Experimental Techniques

Page 6: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

Synthesis of Nanoparticles by PLA

To synthesize Ag (Cu2O @ Cu) NPs by PLA, a high purity silver (copper) slice is placed on the bottom of glass vessel containing 20 ml of distilled water.It is irradiated with focused output of 1064 nm of pulsed Nd:YAG laser (Spectra Physics Inc. USA) operating at fixed energy for 30 minutes. This results a yellow color in Ag (light green in Copper) colloidal solution.

Page 7: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

Characterizations of Nanoparticles

The synthesized nanoparticles are characterized by following techniques

i.UV-Visible absorption spectroscopy: Perkin Elmer Lambda 35 double beam spectrophotometer

ii.Transmission electron microscopy (TEM): Technai G20–stwin electron microscope

iii.X-ray diffraction (XRD) Rikagu, D-Max X-ray diffractometer

Page 8: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

MONOCROMATOR

PMT

Ar+ L A S E R514.5 nm

Sample holder

SERS Experimental Set-up

Page 9: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

Result & Discussion

Page 10: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

Ag Nanoparticles

UV-visible absorption spectrum: The absorption band at ~398 nm is due to SPR of Ag nanoparticles, confirms the formation of pure Ag nanoparticles.

TEM image of Ag sample synthesized at 40 mJ/pulse laser energy confirms formation of nanoparticles with average particle size 2-3 nm.

The inset shows SAED pattern, indicates formation of crystalline nanoparticles

Page 11: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

Cu2O @ Cu Nanoparticles

TEM image of sample synthesized at 40 mJ/pulse laser energy confirms formation of nanoparticles with average particle size 5-8 nm.

UV-visible absorption spectra: The absorption band at ~620 nm are due to SPR of Cu nanoparticles, while absorption in the range 220 - 400 nm are due to interband transition of Cu2O.

Page 12: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

30 35 40 45 50 55 60 65 70 75 80

200

250

300

350

400

450

500

550

O - Cu2O

* - Cu

(20

0)

(11

1)

(31

1)

(22

0)

(11

1)

*

*

oo

oIn

ten

sit

y (

a.u

.)

2 (degree)

The XRD spectrum of the sample synthesized at 40 mJ/pulse laser energy shows diffraction peaks corresponding to Cu2O and Cu, confirms the formation of Cu2O @ Cu nanostructures.

Page 13: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

SERS of Alizarin dye using Ag Nanoparticles

Sample C:Alizarin+ Colloidal Ag NPs+ 1.0 ml solution of 1M NaCl

Sample B:Alizarin+ Colloidal Ag NPs+ 0.5 ml solution of 1M NaCl

Sample A: Alizarin + Colloidal Ag NPs

Alizarin

1203

1611

1786

1987

1826

910

Page 14: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

Observed Wavenumber Assignment

910 (C–H)

1203 (CC)/ (CH)/(CCC)

1611 (C=O)

The enhancement of the Raman signal with addition of Ag NPs and increasing NaCl conc. can be fairly observed from the SERS spectra.

This fact clearly indicates the role of NaCl in signal enhancement by enhancing the rate of aggregation of colloidal Ag NPs.

Observed wavenumbers (cm-1) in Alizarin & assignments

J. Raman Spectrosc. 2006; 37: 993–1002

J. Raman Spectrosc. 2004; 35: 921–927

Page 15: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

SERS of Crystal Violet (CV) dye with Cu2O @ Cu NPs

A4:CV+ Colloidal NPs synthesized at 60 mJ/pulse energy

A3:CV+ Colloidal NPs synthesized at 50 mJ/pulse energy

A2:CV+ Colloidal NPs synthesized at 40 mJ/pulse energy

A1:CV+ Colloidal NPs synthesized at 30 mJ/pulse energy

A0: Diluted pure CV Dye

Page 16: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

It is evident from the SERS spectra that with increase in ablation energy from 30 mJ/pulse (A1) to 40 mJ/pulse (A2), the Raman signals enhance and peaks get resolved.

As the ablation energy increased to 50 mJ/pulse (A3), the SERS signals resolved dramatically. (the peaks appear at 494, 518, 608, 656, 788, 824, 884, 908, 1021, 1399, 1460, 1555, 1598, 1621, 1664, 1682, 1754, 1790, 1826, 1868 and1898 cm-1 ).

This enhancement in Raman signals may be due to increase in NPs concentration.

Further, the SERS signals decreased with the addition of NPs synthesized at 60 mJ/pulse (A4) . ( Peaks appear at 632, 674, 854, 914, 974, 1082, 1154, 1268, 1346, 1454, 1514, and 1796 cm-1).

The decrease in SERS signals is possibly due to increase in size of the NPs.

Page 17: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

The ratios of peaks (λ280/λ574) have highest value for the sample A3, which

shows well resolved SERS spectrum and this confirm the strong interaction between CV and nanoparticles.

The value of ratio (λ280/λ574) decreases drastically for A4, which shows weak

interaction of CV with nanoparticles and thus indicating the possible cause of decrease in SERS signal.

Role of NPs in Enhancement of Raman Signal

280

574

665

Page 18: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

B3:CV+ Colloidal NPs synthesized at 50 mJ/pulse energy+ 0.5ml KI (0.2M)

B2:CV+ Colloidal NPs synthesized at 50 mJ/pulse energy+ 0.5ml KBr (0.2M)

B1:CV+ Colloidal NPs synthesized at 50 mJ/pulse energy+ 0.5ml KCl (0.2M)

Effect of aggregating agent on SERS of CV due to colloidal copper/copper oxide NPs synthesized at 50 mJ/pulse with halide ions (Cl-, Br-, and I-).

Page 19: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

It is evident from these spectra that all three halide ions Cl-, Br-, and I-, enhance the Raman signals of the CV dramatically and Peaks are well resolved.

Sample B1 have well resolved peaks at 433, 630, 677, 765, 829, 898, 927, 1020, 1283, 1421, 1595, 1799, and 1857 cm-1 .

Sample B2 shows peaks at 445, 596, 642, 672, 706, 788, 840, 921, 908, 1002, 1061, 1211, 1247, 1404, 1520, 1613, 1706, 1851, and 1927 cm-1, while the sample B3 has peaks at 451, 555, 596, 636, 672, 718, 979, 1055, 1078, 1119, 1212, 1276, 1368, 1403, 1573, 1752, and 1857 cm-1.

The data show the Raman peaks move towards red with the addition of halide ions from Cl- to Br- to I-.

Page 20: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

The role of Halide ions in the Enhancement of Raman Signal

Peak corresponding to 347 nm appears only with the addition of I-, this confirm the strong interaction between CV and I– ion, which shows well resolved SERS spectrum.

347

570

665

Page 21: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

ConclusionsSERS study of Alizarin Red is done using colloidal Ag NPs as substrate and NaCl as aggregating agent with enhancement with NPs synthesized at 50mj energy.

Raman signal enhancement of Crystal violet using colloidal Cu2O@Cu NPs as substrate is studied. It has been found that the NPs synthesized at 50 mJ/pulse energy not only enhance Raman signals but also show better resolved Raman signals.

The introduction of Cl-, Br-, and I- ions in SERS samples shows considerable enhancement in Raman signals but at different spectral range.

Page 22: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

Acknowledgements Authors are thankful to Prof. B.R. Mehta, I.I.T. Delhi, New Delhi for providing TEM facility and DRDO, New Delhi for research grant.

I am also thankful to DST New Delhi for travel support to attend this symposium.

Page 23: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.
Page 24: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

Chemical Structure of Alizarin

Page 25: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

Chemical Structure of Crystal violet

Page 26: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

Another factor in SERS experiments is the metal solution interface, since it affects the adherence of the adsorbate on the surface.

Page 27: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

nanoparticles

Metal Target

Metal PlasmaDistilled Water

One Laser Pulse

Metal Target

Metal ClusterDistilled water

Metal Target

Step I Step II Step III

Mechanism of the nanoparticles synthesis by laser ablation:

i.Front part of focused laser beam interacts with metal target and evaporates metallic vapors from its surface. These vapors are excited by back part of the laser pulse and creation of hot plasma plume expanding perpendicular to the target surface.

ii.High-temperature and high-pressure plasma above the target after one laser pulse cools down through adiabatic expansion against liquid media and results in the formation of metal clusters

iii. Further cooling of these clusters form metal or metal oxide nanoparticles depending upon chemical interaction of metal with liquid environment.

Page 28: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

I. Electromagnetic (EM) enhancement

The collective excitation of the electron cloud of a conductor is called a plasmon; if the excitation is confined to the near surface region it is called a surface plasmon.

EM enhancement is a consequence of the interaction of incident electric field (from incident radiation) with the electrons in the metal surface, which causes excitation of surface plasmons and, as a result, enhancement of electric field at metal surface (i.e. SERS).

metal

MoleculePlasmons

Incident light SERS Signal

Page 29: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

II. Chemical Enhancement (CE)

CE results from increase in molecular polarizability, due to the charge transfer between metal and sample molecule.

When molecules are adsorbed to the surface, their electronic states can interact with the states in the metal and produce new transitions which causes enhancement of Raman signal.

HOMO: Highest occupied molecular orbit

LUMO: Lowest unoccupied molecular orbit

Page 30: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

Observed wavenumbers (cm-1) in CV & assignments

Observed Wave-number

Assignment Observed Wavenumber

Assignment

450 C+ - Ph and ring skeletal out-of-plane vibration

764 C – H out-of plane bending

555 ring skeletal vibrations of radical orientation

787 C – H out-of-plane bending

631 ring skeletal vibrations of radical orientation

824 C – H out-of-plane bending

636 ring skeletal vibrations of radical orientation

1346 N – Ph stretching vibrations

908 ring skeletal vibrations of radical orientation

1382 N – Ph stretching vibrations

914 ring skeletal vibrations of radical orientation

1399 N – Ph stretching vibrations

979 ring skeletal vibrations of radical orientation

1598 ring C-C stretching

986 ring skeletal vibrations of radical orientation

1621 ring C-C stretching

718 C – H out-of-plane bending

Page 31: R. Gopal & R.K. Swarnkar Laser Spectroscopy & Nanomaterials Lab. Centre of Advanced Studies Department of Physics University of Allahabad, INDIA STUDY.

UV-visible absorption spectrum shows red shift due to aggregation of Ag NPs.

405

525

427