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Technical Notes


101 - Principle of SPR detection - intensity profile and shift of the SPR angle

When a light beam impinges onto a metal film at a specific (resonance) angle, the surface plasmons are set to resonate with the light. The resonance results in the absorption of light. In the widely used Kretschmann configuration, a beam is focused onto the metal film. The focused light provides a range of incident angles, and the reflected beam will cover the same range of the angles while the projection of the beam forms a band. When the SPR occurs within the spread angles, a dark line will appear in the band. An intensity profile of this band is plotted against the range of angles as shown in Figure 1.

BI-SPR Technology . Flow Injection SPR . Electrochemical SPR . Gas Phase SPR

 
     
  Figure 1. Principle of SPR detection in the mode of measuring the SPR angular shift.  
This profile is often used in a typical SPR experiment to indicate that the metal film (or the solution above the metal film) matches the SPR resonance condition, and that the apparatus is set up properly. However, the actual measurement of molecular adsorption kinetics is only related to the shift of the absorption (SPR) dip corresponding to the SPR angle change (Figure 2). One has to sacrifice the resolution of the measurement by acquiring the whole intensity profile curves and comparing them to find the shift of the dip (minimum).
























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Figure 2. A light is beamed upon a metal film through a prism and the reflected beam image shows a dark line due to SPR. The intensity profile of the reflected beam exhibits a dip or minimal intensity at the resonance angle. An SPR experiment measures the position shift of the dip (the angle shift) upon molecular adsorption, and this shift represents the adsorption kinetics when plotted as a function of time.


Biosensing Instrument Incorporated uses a different approach to detect the SPR angle change by using a position-sensitive detector to detect the SPR absorption dip shift. Since it only measures the position shift of the dip, it offers a highly sensitive detection scheme to measure extremely small angle changes of the SPR. As long as the SPR angle resides inside the angle spread, the system delivers exceptionally high angular resolution in its measurement.

Even though intensity profile is commonly used for demonstrating the proper alignment and the setup of an SPR system, it only offers limited status check of a metal film at a single position. For a dual-channel detection scheme, a single intensity profile check is not sufficient to ensure that the system is in proper SPR detection condition. One has to ensure that all the illuminated areas of the metal film are in good condition. BI-SPR instruments provides the user a simple but sufficient solution by projecting the SPR absorption dip onto a screen that can be visualized. By examining the quality of the dark line (as shown in figure 3-5), one could ensure that all conditions of the SPR are met and a successful experiment can be conducted.

   
Figure 3. A good metal film gives a clean and straight SPR dark line in air (left) and solution (right).
 
Figure 4. A bad or contaminated film gives fuzzy and indistinct dark line.
 
Figure 5. A trapped air bubble underneath of the metal film sensor will break the dark line. However, at the drawn line, dark line will still gives a good intensity profile of the SPR.


As illustrated in Figure 3, a good metal film gives a well-defined, clean, and straight dark line. This guarantees a good intensity profile at any point along the dark line. Figure 4 and 5 demonstrated that a partially contaminated metal film can still give a reasonable intensity profile of SPR at a given point. However, it will not lead to a reliable measurement, since the film quality across a large area is bad.


   
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