Scanning SFG Spectrometer

Picosecond Scanning Sum Frequency Generation (SFG) Vibrational Spectrometer

In order to get SFG spectrum during measurement wavelength of narrowband mid-IR pulse is changed point-by-point throughout the range of interest.  Narrowband SFG signal is recorded by the time-gated photomultiplier.

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Advantages

  • Sensitive and selective to the orientation of molecules in the surface layer
  • Intrinsically surface specific
  • Selective to adsorbed species
  • Sensitive to submonolayer of molecules
  • Applicable to all interfaces accessible to light
  • Nondestructive
  • Capable of high spectral and spatial resolution

Applications

  • Investigation of surfaces and interfaces of solids, liquids, polymers, biological membranes and other systems
  • Studies of surface structure, chemical composition and molecular orientation
  • Remote sensing in hostile environment
  • Investigation of surface reactions under real atmosphere, catalysis, surface dynamics
  • Studies of epitaxial growth, electrochemistry, material and environmental problems

Sum Frequency Generation Vibrational Spectroscopy

Sum Frequency Generation Vibrational Spectroscopy (SFG-VS) is powerful and versatile method for in-situ investigation of surfaces and interfaces. In SFG-VS experiment a pulsed tunable infrared IR (ωIR) laser beam is mixed with a visible VIS (ωVIS) beam to produce an output at the sum frequency (ωSFG = ωIR + ωVIS). SFG is second order nonlinear process, which is allowed only in media without inversion symmetry. At surfaces or interfaces inversion symmetry is necessarily broken, that makes SFG highly surface specific. As the IR wavelength is scanned, active vibrational modes of molecules at the interface give a resonant contribution to SF signal. The resonant enhancement provides spectral information on surface characteristic vibrational transitions.

Vibrational sum frequency generation (SFG) spectroscopy offers several important advantages over traditional spectroscopy methods for the molecular level analysis of interfaces, including surface sensitivity, vibrational specificity, and the possibility to extract detailed information on the ordering and orientation of molecular groups at the interface by analysis of polarization-dependent SFG spectra.

SFG signal generation diagram (a) and the molecular energy level diagram for the SFG process (b)

SFG signal generation diagram (a) and the molecular energy level diagram for the SFG process (b).

Spectra examples

Comparison of Narrowband and Broadband SFG Spectrometers

Narrowband picosecond scanning SFG spectrometer

In order to get SFG spectrum during measurement wavelength of narrowband mid-IR pulse is changed point-by-point throughout the range of interest.  Narrowband SFG signal is recorded by the time-gated photomultiplier. Energy of each mid-IR, VIS and SFG pulse is measured. After the measurement, the SFG spectrum can be normalised according to IR and VIS energy. Spectral resolution is determined by the bandwidth of the mid-IR light source. The narrower mid-IR pulse bandwidth, the better the SFG spectral resolution. Separate vibrational modes are excited during the measurement.

Broadband femtosecond SFG spectrometer

A broadband mid-IR pulse is mixed with a narrowband VIS pulse. The result is broadband SFG spectrum which is recorded using a monochromator and a sensitive CCD camera. The full spectrum is acquired simultaneously by integrating signal over time. Spectral resolution is determined by the bandwidth of the VIS pulse and on the monochromator-camera combination. The narrower the bandwidth of VIS pulse, the better the SFG spectral resolution.

Diagram of Narrowband picosecond scanning SFG spectrometer.

Diagram of Narrowband picosecond scanning SFG spectrometer.

Diagram of Broadband femtosecond SFG spectrometer

Diagram of Broadband femtosecond SFG spectrometer.

Comparison of different SFG spectrometres

Narrowband Picosecond Scanning SpectrometerBroadband Femtosecond High Resolution Spectrometer
Narrowband mid-IR excitation, only one band is excited. Coupled states can be separated.Simultaneous exsitation and recording of broad vibration spectrum with high resolution.
High mid-IR pulse energy. Less influence of IR absorbtion in the air.High mid-IR intensity at low pulse energy – suitable for biological or other water containing samples.
No reference spectrum needed, IR energy measured at each spectral point.Optically coupled IR and VIS channels. Reduced complexity and increased stability of the system.

Spectra examples

Features and Design

Picosecond Scanning Sum Frequency Generation (SFG) Vibrational Spectrometer

Picosecond Scanning Sum Frequency Generation (SFG) Vibrational Spectrometer.

System Components

  • Picosecond mode-locked
  • Nd:YAG laser and optical parametric generator in one unit
  • Spectroscopy module with:
    – PMT based signal detectors
    – Data acquisition system
    – Dedicated LabView® software package for system control
  • Fast wavelength scan (sweep)

The SFG spectrometer developed by Ekspla engineers is a nonlinear spectrometry instrument, convenient for everyday use. Ekspla manufactures SFG spectrometers, which are used by chemists, biologists, material scientists, and physicists. The spectrometer has many features that help to set up measurements and to make successful vibrational spectroscopy studies. For chemical and biochemical laboratories, this makes the Ekspla SFG spectrometer a reliable workhorse with a broad spectral region, automatically tuned from 625 to 4300 cm‑1, a high spectral resolution (3 cm‑1), and easily controlled adjustment of polarisation optics.

The new SFG classic spectrometer consist of two units: laser light source PT501 and spectroscopy module.

Schematic layout of SFG Classic spectrometer.

Schematic layout of SFG Classic spectrometer.

The Ekspla SFG system is based on a mode-locked Nd:YAG laser with a 29 ps pulse duration, 100 Hz repetition rate. The VIS channel of the SFG spectrometer consists of part of a laser output beam, usually with doubled frequency (532 nm) up to 0.3 mJ. The main part of the laser radiation goes to an optical parametric generator (OPG) with a difference frequency generation (DFG) extension. The IR channel of the spectrometer is pumped by the DFG output beam with energy in the range of ~40 – 200 μJ. Infrared light can be tuned in a very broad spectral range from 2.3 up to 16 μm. The bandwidth is 3 cm‑1 and it is one of the main factors of SFG spectrometer spectral resolution. The second beam (VIS) is also narrowband at <2 cm‑1. The spectrometer signal detection system has a temporal gate. It significantly reduces accumulative noise and ambient light influence, which allows to use spectrometer even in a brightly illuminated room. The spectrometer does not have any acoustic noise because the laser is pumped by light emiting laser diodes.

The spot size of the IR beam is adjustable. In this way, the appropriate energy density is achieved in order to avoid damaging or modifying the sample. Spectrum scanning, polarisation control and VIS beam attenuation are controlled from a computer. The spectrometer has a motorized polarisation switch for the IR, optionaly for the VIS, and optionaly the generated SFG light beams. Energy detectors continuously monitor the energy of the VIS and mid-IR laser pulses, so IR energy is recorded at each measurement point. This makes it possible to normalise the resulting SFG vibrational spectrum.

Fast wavelength scan (sweep) allows fast access to a wide spectral range. Using time-synchronised motor positions enables fast and smooth wavelength tuning which allows users to scan the full range in just a few seconds or access specific wavelengths within 0.3 seconds.

A large sample compartment can be customised and enables the use of various extensions and additional instruments for simultaneous control of the sample conditions, including a Langmuir-Blodgett trough for air/water and lipid/air interface studies, temperature and humidity-controlled cells, and other instruments.

The spectrometer is safe to use: all high energy pulsed beams are enclosed. In addition, the sample area also has a special cover. During the measurements, it is possible to close the sample compartment so that radiation cannot penetrate outside. The automatic change of polarisation and energy attenuation makes it possible to perform measurements without opening the spectrometer. Laser safety precautions are required only for the alignment of the laser beams on the studied surface.

Modification

  • Double resonance SFG spectrometer – allows investigation of vibrational mode coupling to electron states at a surface
  • Phase sensitive SFG spectrometer – allows measurement of the complex spectra of surface nonlinear response coefficients

Options

  • Single or double wavelength VIS beam: 532 nm and/or 1064 nm
  • One or two detection channels: main signal and reference
  • Second harmonic generation surface spectroscopy option
  • Motorized polarisation control for VIS and SFG beams
  • Larger sample compartment to accomodate Langmuir through
  • Simultaneous measurement of s and p polarisation of SFG signal

Both IR and VIS wavelengths are tunable in Double resonance SFG spectrometer model.

This two-dimensional spectroscopy is more selective than single resonant SFG. Double resonant SFG allows investigation of vibrational mode coupling to electron states at a surface.

Double resonance enables the use of another wavelength for VIS beam if the sample has strong absorption at 532 nm and 1064 nm. A range 420 – 680 nm is typically used for VIS beam.

The second tunable laser system is used for the double-resonance SFG. Two laser systems PT501 and PT401 are opticaly synchronised.

* Laser is located in the PT501 system. System PT401 can not operate separately from PT501.

Schematic layout of SFG double resonsnce spectrometer.

Schematic layout of SFG double resonsnce spectrometer.

A phase sensitive spectrometer allows the measurement the phase of nonlinear susceptibility χ(2). Reference and test samples are used and the SFG phase difference between them is scanned. The real and imaginary parts of second order susceptibility are calculated from the experimental results. Such an approach enables the unambiguous determination of the orientation of molecular groups at the interface.

Phase-sensitive SFG spectrometer software.

Phase-sensitive SFG spectrometer software.

Interferograms of AZO (azophenylcarbazole) dyes on the Au surface and fitted SF spectra with amplitude and phase distinguished.

In conventional SFG-VS intensity of SF signal is measured. It is proportional to the square of second order nonlinear susceptibility ISF ~ | χ(2) |2. However, χ(2) is complex, and for complete information, we need to know both the amplitude and the phase. This will allow us to determine the absolute direction in which the bonds are pointing and characterize their tilt angle with respect to the surface. Measurement of the phase of an optical wave requires an interference scheme. Mixing the wave of interest with a reference wave of known phase generates an interference pattern, from which the phase of the wave can be deduced.

In practice Phase-sensitive SFG experimental setup includes two samples generating SF signal simultaneously. One sample (usually called local oscillator) has well known and flat spectral response. Second one is investigated sample. The excitation beams are directed to first sample, where SFG beam is generated. Later all three beams are retranslated to the second sample, where another SFG beam is generated. Due to electromagnetic waves coherence both SFG beam are interfering. Setup contains the phase modular located on the SFG beam path between samples. We are able to change the phase of SFG beam by rotating it. This way we are recording two-dimensional interfererogram with wavelength and phase shift on x and y axis. Using fitting algorithms we are able to calculate the amplitude and phase of SF signal.

Interference measurements of SFG signals from reference sample and the investigated sample for Phase-sensitive configuration.

Switchable setup. Phase Sensitive / “Classic” Top configuration.
Switch: VIS beam manual. IR mirror mount is motorised, lens positioning stage is manual.
Path length to the sample is same in all configuration
Motorised polarisation control.
VIS beam 532 nm. IR 2.3 – up to 16 µm.

Options

  • Spectrometer has “Classic” and “Phase-sensitive” properties:
  • Easy switching between setups
  • Adjustable spot size for classic configuration

Polarisation control

Simultaneous measurement of S and P polarisation

S and P polarisation of the SFG signal are detected during the same measurement in the dual polarisation detection system.

Motorized polarisation control of SFG, VIS, IR

The SFG spectrometer has a motorized polarisation switch for the IR, VIS, and the generated SFG light beams. The automatic change of polarisation and energy attenuation makes it possible to perform measurements without opening the spectrometer.

  • Motorized switching of IR – standard
  • Motorized control in small steps of SFG, VIS – optionally

SFG Spectrometer Accessories

  • Six axis sample holder
  • Sealed temperature controlled sample chamber
  • Larger sample area – space for Langmuir trough
  • Motorisation of polarisation control of VIS and IR beams, polarisation analyser for SFG signal

Specifications

Version 1)SFG ClassicSFG Double resonanceSFG Phase sensitive
System (general)
Spectral range625 – 4300 cm‑1625 – 4300 cm‑1 (VIS 532 nm)
1000 – 4300 cm‑1 (VIS 420 – 680 nm)
1000 – 4300 cm‑1
Spectral resolution< 3 cm‑1< 3 cm‑1< 3 cm‑1
Spectra acquisition methodScanning and fast wavelength sweepScanning and fast wavelength sweepScanning and fast wavelength sweep
Sample illumination geometryTop side, reflectionTop side, reflectionTop side, reflection
Incidence beams geometryCo-propagating, non-colinearCo-propagating, non-colinearCo-propagating, non-colinear
Incidence anglesFixed, VIS ~60 °, IR ~55 ° (optional: tunable)Fixed, VIS ~60 °, IR ~55 ° (optional: tunable)Fixed, VIS ~60 °, IR ~55 °
VIS beam wavelength532 nm532 nm and
tunable 420 – 680 nm
532 nm
Polarization (VIS, IR, SFG)Linear, selectable “s” or “p”, purity > 1:100Linear, selectable “s” or “p”, purity > 1:100Linear, selectable “s” or “p”, purity > 1:100
IR Beam spot on the sampleAdjustable, ~200 – 600 µmAdjustable, ~200 – 600 µmFixed
SensitivityAir-water interface spectraAir-water interface spectraSolid sample spectra
Laser light source 2)
ModelPT501-SHPT501-SHPT501-SH
Pulse duration29 ± 5 ps29 ± 5 ps29 ± 5 ps
Pulse repetition rate100 Hz100 Hz100 Hz
UV-VIS source for
Double resonance SFG
PT401
Physical characteristics (footprint)
Standard1300 × 1200 mm1800 × 1200 mm1400 × 1200 mm
Version 1)SFG ClassicSFG Double resonanceSFG Phase sensitive
  1. Due to continuous improvement, all specifications are subject to change without advance notice.
  2. Laser is optimised for pumping parametrical generator, maximum output energy may be different than specified for stand alone application.

Publications

Hydrogen bonding interactions of H₂O and SiOH on a boroaluminosilicate glass corroded in aqueous solution

D. Ngo, H. Liu, Z. Chen, H. Kaya, T. J. Zimudzi, S. Gin et al., npj Materials Degradation 4 (1), 1 (2020). DOI: 10.1038/s41529-019-0105-2.

Structure Determination of Hen Egg-White Lysozyme Aggregates Adsorbed to Lipid/Water and Air/Water Interfaces

S. Strazdaite, E. Navakauskas, J. Kirschner, T. Sneideris, and G. Niaura, Langmuir 36 (17), 4766-4775 (2020). DOI: 10.1021/acs.langmuir.9b03826.

Aggregation states of poly (4-methylpentene-1) at a solid interface

K. Yamamoto, D. Kawaguchi, K. Sasahara, M. Inutsuka, S. Yamamoto, K. Uchida et al., Polymer Journal 51 (2), 247-255 (2019). DOI: 10.1038/s41428-018-0134-7.

Reconfiguration of interfacial energy band structure for high-performance inverted structure perovskite solar cells

M. Zhang, Q. Chen, R. Xue, Y. Zhan, C. Wang, J. Lai et al., Nature communications 10 (1), 4593 (2019). DOI: 10.1038/s41467-019-12613-8.

Segregation of an amine component in a model epoxy resin at a copper interface

M. Aoki, A. Shundo, K. Okamoto, T. Ganbe, and K. Tanaka, Polymer Journal 51 (3), 359-363 (2019). DOI: 10.1038/s41428-018-0129-4.

Vibrational Relaxation Lifetime of a Physisorbed Molecule at a Metal Surface

S. Kumar, H. Jiang, M. Schwarzer, A. Kandratsenka, D. Schwarzer, and A. M. Wodtke, Phys. Rev. Lett. 123, 156101 (2019). DOI: 10.1103/PhysRevLett.123.156101.

Heavy Anionic Complex Creates a Unique Water Structure at a Soft Charged Interface

W. Rock, B. Qiao, T. Zhou, A. E. Clark, and A. Uysal, The Journal of Physical Chemistry C 122 (51), 29228-29236 (2018). DOI: 10.1021/acs.jpcc.8b08419.

High-performance graphdiyne-based electrochemical actuators

C. Lu, Y. Yang, J. Wang, R. Fu, X. Zhao, L. Zhao et al., Nature communications 9 (1), 752 (2018). DOI: 10.1038/s41467-018-03095-1.

Vibrational fingerprint of localized excitons in a two-dimensional metal-organic crystal

M. Corva, A. Ferrari, M. Rinaldi, Z. Feng, M. Roiaz, C. Rameshan et al., Nature Communications , 4703 (2018). DOI: 10.1038/s41467-018-07190-1.

A structural and temporal study of the surfactants behenyltrimethylammonium methosulfate and behenyltrimethylammonium chloride adsorbed at air/water and air/glass interfaces using sum frequency generation spectroscopy

S. A. Goussous, M. T. L. Casford, S. A. Johnson, and P. B. Davies, Journal of Colloid and Interface Science 488, 365-372 (2017). DOI: 10.1016/j.jcis.2016.10.092.

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