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Characterizing Gold Nanorods by Utilizing VV and VH Modes in DLS

2024-06-28Application Note

This application note emphasizes the combined use of VV and VH modes in dynamic light scattering (DLS) measurements, enabling a thorough analysis of anisotropic particles such as gold nanorods. The BeNano 180 Zeta Pro accurately measures both translational and rotational diffusion, offering detailed insights into the particles' morphology and dynamics.

 

Product BeNano Series (BeNano 180 Zeta Pro)
Industry Nanomaterials
Sample Gold Nanorods
Measurement Type Particle Size
Measurement Technology Dynamic light scattering (DLS)

 

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Introduction 

Figure-1-SEM-Images-of-Gold-Nanorods

Figure 1. SEM Images of Gold Nanorods

 

Some samples exhibit anisotropic shapes such as rods or disks rather than spherical forms. In dynamic light scattering (DLS) measurements, the diffusion behavior of these samples involves not only translational diffusion but also significant rotational diffusion. For these samples, it is essential to perform DLS measurements using both VV and VH modes.

 

  • VV mode uses a vertically polarized laser source and a vertical polarizer in the detection path, collecting only vertically polarized scattered light.
  • VH mode uses a vertically polarized laser source and a horizontal polarizer in the detection path, collecting only horizontally polarized scattered light. VH mode is also known as depolarized dynamic light scattering (DDLS).

 

Combining the results from VV and VH modes allows for the determination of the rotational diffusion coefficient Dr in anisotropic systems, providing more information about the sample's morphology and motion.

 

In this application note, the BeNano 180 Zeta Pro is used to measure the translational and rotational diffusion of gold nanorods dispersed in water.

BeNano 180 Zeta Pro 

 

Experimental 

The gold nanorods were measured using the BeNano 180 Zeta Pro with a built-in temperature control system, set to a default test temperature of 25°C ± 0.1°C.

Figure 2. Multifunctional Micro-volume Cells for VH (left) and VV (right) Modes

Figure 2. Multifunctional Micro-volume Cells for VH (left) and VV (right) Modes

 

Using the micro-volume cells, only 16 μL of the sample is needed, significantly saving valuable sample. The samples were measured at least three times to ensure reproducibility and to calculate the standard deviation of the results.

 

Results and Discussion 

VV and VH mode tests were performed at a 90° angle. The DLS results are shown below:

Figure 3. 90° VV Mode Correlation Functions of Multiple Tests

Figure 3. 90° VV Mode Correlation Functions of Multiple Tests

Figure 4. 90° VH Mode Correlation Functions of Multiple Tests

Figure 4. 90° VH Mode Correlation Functions of Multiple Tests

 

The derived formula from literature shows that the light intensity correlation function for rod-shaped samples under VV and VH test conditions is:

derived-formula

where Γ=2DTq2, Δ=12Dr , q is the scattering vector. In the VV mode, the correlation function includes contributions from both translational and rotational diffusion, leading to multiple  exponential decays. In the VH mode, the correlation function shows a single exponential decay. This matches the observed correlation functions in Figures 3 and 4.

 

Based on theoretical derivations, the field intensity correlation functions for VV and VH modes are as follows:

derived-formula

Figure 5. Double Exponential Fitting of g1VV Correlation Function

Figure 5. Double Exponential Fitting of g1VV Correlation Function

 

By calculating the natural logarithm of g1VH and using polynomial fitting, one can obtain DTq2+6Dr. Double exponential fitting of g1VV yields both DTq2+6Dr and DTq2. The results are summarized in the table below:

 

Table 1. Fitting results from VV and VH modes

Item Method Result
DTq2+6Dr (1/s) Polynomial fit of g1VH 66935.67
DTq2+6Dr (1/s) Fast decay in VV mode 63260.50
D(nm2 /ms) Slow decay in VV mode 2941.07
Dr (1/ms) Combined fast and slow decay in VV mode 10.58

 

Table 1 shows that the results from VV and VH modes are consistent, ultimately providing the rotational diffusion coefficient Dr for the gold nanorods.

 

Conclusion 

The combined use of VV and VH modes in dynamic light scattering (DLS) tests allows for comprehensive analysis of anisotropic particles like gold nanorods. The BeNano 180 Zeta Pro effectively measures both translational and rotational diffusion, providing detailed insights into the particles' morphology and motion. This approach ensures accurate characterization and enhances understanding of such complex systems.

 

About the Authors

Bettersize-application-engineer-Zhibin-Guo Zhibin Guo

Application Manager @ Bettersize Instruments
Bettersize-Chief-Product-Officer-Hui-Ning

 Dr. Ning

Chief Product Officer @ Bettersize Instruments

 

BeNano 180 Zeta Pro

 Nanoparticle Size and Zeta Potential Analyzer

  • Measurement range: 0.3nm - 15μm
  • Minimum sample volume: 3μL
  • High-concentration sample measurement: Backscattering (173°) technology
  • Automatic pH and temperature trend analysis


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