Vista 75: Compact System for Nano-IR Analysis

The Vista 75 delivers precise and versatile Nano-IR Analysis in a compact, user-friendly system.

Vista 75: Small and Mighty

Accessible Design

Convenient sample access and a single-handed AFM head clamp enable quick and simple tip and sample exchanges. Its lightweight, removable enclosure, and open design simplify complex optical alignments.

Quick-Change Optics

Pre-aligned optics allow seamless switching between PiFM + PiF-IR, s-SNOM, and Raman modes.

Self-Contained System

Designed for standard lab conditions, the Vista 75 features integrated vibration isolation and a temperature-controlled acoustic enclosure with dry air, eliminating the need for a specialized environment.

75 mm Sample Stage Travel

Sample size is no longer a limitation—if it fits on the stage, the Vista 75 can deliver results.

Dynamic Laser Control

The advanced optical multiplexer automatically manages alignments, polarization, and normalization, ensuring effortless laser control.

Ultimate Spectro-Nanoscopy

Photo-induced force microscopy (PiFM) and photo-induced force infrared (PiF-IR) spectroscopy represent the forefront of nano-IR techniques.

Exceptional AFM Performance

Equipped with an 80 µm (optional 100 µm) XY-scanner and a dual Z-feedback system, the integrated AFM offers exceptional performance.

Vista 75: Compact System for Nano-IR Analysis

Image Credit: Molecular Vista

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Scientific Principles PiFM & PiF-IR

A pulsed and tunable IR laser is focused onto the apex of a metal coated AFM tip. The laser is modulated at a frequency carefully calculated based on the resonance frequencies of the cantilever.

Figure 1. A pulsed and tunable IR laser is focused onto the apex of a metal coated AFM tip. The laser is modulated at a frequency carefully calculated based on the resonance frequencies of the cantilever. Image Credit: Molecular Vista

The metal-coated AFM tip acts as an antenna and creates a highly local enhanced field (yellow). This field locally polarizes the sample, resulting in an attractive force whose magnitude depends on the absorption strength of the sample

Figure 2. The metal-coated AFM tip acts as an antenna and creates a highly local enhanced field (yellow). This field locally polarizes the sample, resulting in an attractive force whose magnitude depends on the absorption strength of the sample. Image Credit: Molecular Vista

One resonance of the cantilever is used to detect the PiFM signal. Simultaneously, another resonance is used to collect the standard AFM topography and phase in a non-contact manner (no tip/sample contamination).

Figure 3. One resonance of the cantilever is used to detect the PiFM signal. Simultaneously, another resonance is used to collect the standard AFM topography and phase in a non-contact manner (no tip/sample contamination). Image Credit: Molecular Vista

The depth of the tip-enhanced illumination depends heavily on the spacing between the tip and the sample. By detecting the attractive forces in non-contact mode, the measurement is made extremely sensitive – capable of detecting monolayers of material

Figure 4. The depth of the tip-enhanced illumination depends heavily on the spacing between the tip and the sample. By detecting the attractive forces in non-contact mode, the measurement is made extremely sensitive – capable of detecting monolayers of material. Image Credit: Molecular Vista

The Result

PiF-IR nanoscale spectra are made by measuring the strength of the attractive photo-induced forces as a function of wavenumber. PiFM chemical maps are created by scanning the surface with a fixed-wavenumber to measure absorption strength as a function of position. The color layer over the AFM topography is three fixed-wavenumber PiFM images combined.

Figure 5. PiF-IR nanoscale spectra are made by measuring the strength of the attractive photo-induced forces as a function of wavenumber. PiFM chemical maps are created by scanning the surface with a fixed-wavenumber to measure absorption strength as a function of position. The color layer over the AFM topography is three fixed-wavenumber PiFM images combined. Image Credit: Molecular Vista

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PiFM Chemical Mapping

Reveal Hidden Structure in Color

3D visualization of the AFM topography of a cell wall from an ultra-thin cross section of spruce wood. An overlay of two PiFM images shows the chemical composition of the surface where lignin and cellulose mix. This PiFM overlay reveals how the materials are distributed, and it shows how some of the topographic features are related to the local chemistry. Scan dimensions: 1 µm × 1 µm × 0.034 µm.

Figure 6. 3D visualization of the AFM topography of a cell wall from an ultra-thin cross section of spruce wood. An overlay of two PiFM images shows the chemical composition of the surface where lignin and cellulose mix. This PiFM overlay reveals how the materials are distributed, and it shows how some of the topographic features are related to the local chemistry. Scan dimensions: 1 µm × 1 µm × 0.034 µm. Image Credit: Molecular Vista

Sub-5 nm Spatial Resolution

A zoomed-in region of the spruce wood cell wall. At only 150 nm square, this scan area is over 50 times smaller than in figure 6! PiFM images show the chemical distribution of lignin and cellulose on the surface. A line trace plotting the intensity of the data in the green image shows an IR spatial resolution of less than 5 nm. Notice how the PiFM images bring the topography alive with precise chemical detail while the topography itself is unremarkable. Scan dimensions: 150 nm × 150 nm × 10.5 nm.

Figure 7. A zoomed-in region of the spruce wood cell wall. At only 150 nm square, this scan area is over 50 times smaller than in figure 6! PiFM images show the chemical distribution of lignin and cellulose on the surface. A line trace plotting the intensity of the data in the green image shows an IR spatial resolution of less than 5 nm. Notice how the PiFM images bring the topography alive with precise chemical detail while the topography itself is unremarkable. Scan dimensions: 150 nm × 150 nm × 10.5 nm. Image Credit: Molecular Vista

PiF-IR Nano-Spectroscopy

Single-Molecule-Level Sensitivity

This sample was intended to be a uniform monolayer of peptoid molecules; however, initial PiF-IR analysis indicated that actual peptoid coverage was very sparse. Therefore, a PiFM image was taken at 1633 cm−1 which should highlight any peptoid molecules present. This image reveals tiny peptoid fragments on the surface. A PiF-IR spectrum taken on one of those points shows the characteristic peak at 1633cm−1 despite the peptoid fragment being only 1.7 nm tall! The black spot in the green PiFM image shows that the fragment is sitting on top of the substrate material. Scan dimensions: 500 nm × 500 nm × 1.7 nm.

Figure 8. This sample was intended to be a uniform monolayer of peptoid molecules; however, initial PiF-IR analysis indicated that actual peptoid coverage was very sparse. Therefore, a PiFM image was taken at 1633 cm−1 which should highlight any peptoid molecules present. This image reveals tiny peptoid fragments on the surface. A PiF-IR spectrum taken on one of those points shows the characteristic peak at 1633cm−1 despite the peptoid fragment being only 1.7 nm tall! The black spot in the green PiFM image shows that the fragment is sitting on top of the substrate material. Scan dimensions: 500 nm × 500 nm × 1.7 nm. Image Credit: Molecular Vista

Excellent Agreement with FTIR

On homogeneous samples, PiF-IR spectra agree with FTIR extremely well

Figure 9. On homogeneous samples, PiF-IR spectra agree with FTIR extremely well. Image Credit: Molecular Vista

Analyze Organic and Inorganic Materials

Both organic and inorganic samples can be analyzed equally well using PiFM and PiF-IR. Here, a PS-b-PMMA block copolymer has undergone sequential infiltration synthesis to produce aluminum oxides in the PMMA block. The sample was exposed to a vapor of trimethyl aluminum, which should only react with carbonyl groups in the PMMA. Subsequent exposure to water vapor converts the trimethyl aluminum into aluminum oxide. PiFM analysis after this process confirms the block-selective infiltration by the presence of a new broad peak from 800 to 1100 cm−1 (not shown). A PiFM image taken at 900 cm−1 (yellow image) highlights the infiltrating alumina in the PMMA blocks, demonstrating the exceptional resolution of PiFM chemical mapping even on inorganic samples. Scan dimensions: 500 nm × 500 nm × 5.5 nm.

Figure 10. Both organic and inorganic samples can be analyzed equally well using PiFM and PiF-IR. Here, a PS-b-PMMA block copolymer has undergone sequential infiltration synthesis to produce aluminum oxides in the PMMA block. The sample was exposed to a vapor of trimethyl aluminum, which should only react with carbonyl groups in the PMMA. Subsequent exposure to water vapor converts the trimethyl aluminum into aluminum oxide. PiFM analysis after this process confirms the block-selective infiltration by the presence of a new broad peak from 800 to 1100 cm−1 (not shown). A PiFM image taken at 900 cm−1 (yellow image) highlights the infiltrating alumina in the PMMA blocks, demonstrating the exceptional resolution of PiFM chemical mapping even on inorganic samples. Scan dimensions: 500 nm × 500 nm × 5.5 nm. Image Credit: Molecular Vista

Orientation Discrimination

Similar to polarized FTIR, PiF-IR spectra are orientation sensitive due to the tip-enhanced field. The PiF-IR spectra above were acquired at different crystal faces on a vitamin C sample. They exhibit the local IR bands associated with the specific crystal faces. The average of these three distinct local PiF-IR spectra compare nicely with the bulk FTIR spectrum, which is the equivalent of an ensemble average of billions of PiF-IR spectra. Scan dimensions: 640 nm × 640 nm × 1025 nm

Figure 11. Similar to polarized FTIR, PiF-IR spectra are orientation sensitive due to the tip-enhanced field. The PiF-IR spectra above were acquired at different crystal faces on a vitamin C sample. They exhibit the local IR bands associated with the specific crystal faces. The average of these three distinct local PiF-IR spectra compare nicely with the bulk FTIR spectrum, which is the equivalent of an ensemble average of billions of PiF-IR spectra. Scan dimensions: 640 nm × 640 nm × 1025 nm. Image Credit: Molecular Vista

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Comparisons

Comparing Surface Analytical Techniques

Table 1. PiFM & PiF-IR bring molecular analysis to the realm of true nanoscale resolution, providing both IR absorption spectra and chemical mapping with sub-5 nm spatial resolution and monolayer sensitivity, complementing XPS or ToF-SIMS in any high-end lab. *For SEM and TEM, EDS measurements are not as high resolution as is possible for imaging. Source: Molecular Vista

  PiFM &
PiF-IR
Raman FTIR TOF-
SIMS
XPS TXRF SEM/
EDS
TEM Auger
Species
Detected
Molecular Molecular Molecular Molecular Molecular Elemental Elemental Elemental Elemental
Chemical
Mapping
Yes Yes Yes Yes Yes Yes Yes Yes Yes
Lateral
Resolution
Sub 5
nm
> 0.5
μm
> 10
μm
100
nm
Sub 5
μm
~10
mm
1 nm
*0.5 μm
EDS
0.2 nm
*1 – 20 nm
EDS
8
nm
Depth
Probed
20 nm
& bulk
> 500
nm
1
μm
1
nm
10
nm
10
nm
1
μm
~100
nm
10
nm

 

Vista 75 Specifications

Source: Molecular Vista

Stage and scanner
Sample stage travel 75 mm, max sample 140 mm square.
Scan size 80 × 80 μm (100 × 100 μm option).
Dual Z feedback 12 μm z-scanner with 600 nm fast z-scanner provides both high bandwidth and a large z-range.
Physical requirements
Table size 1.2 m × 1.8 m (4 ft × 6 ft) optical breadboard recommended
Enclosure About 13 kg, removable, acoustic insulation, temperature controlled with dry air.
Functionality
Imaging modes nc-AFM, PiFM, KPFM, cAFM, nano DMA, FvD (force vs distance) mapping, Raman, s-SNOM.
Spectroscopy modes PiF-IR, FvD, Raman.
PiF Laser options QCL (770 – 1840, 1995 – 2395 cm−1), OPO/DFG (590 – 2050, 2250 – 4400, 5000 – 7000 cm−1).
Depth Probed 20 nm in surface mode & greater than 100 nm in bulk mode.

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