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Dual-polarization interferometry

From Wikipedia, the free encyclopedia
Analytical technique that probes molecular layers adsorbed to the surface of a waveguide

Dual-polarization interferometry (DPI) is an analytical technique that probes molecular layers adsorbed to the surface of awaveguide using theevanescent wave of alaser beam. It is used to measure theconformational change in proteins, or other biomolecules, as they function (referred to as theconformation activity relationship).

Instrumentation

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DPI[1] focuses laser light into two waveguides. One of these functions as the "sensing" waveguide having an exposed surface while the second one functions to maintain a reference beam. A two-dimensionalinterference pattern is formed in the far field by combining the light passing through the two waveguides. The DPI technique rotates thepolarization of the laser, to alternately excite two polarization modes of the waveguides. Measurement of the interferogram for both polarizations allows both therefractive index and the thickness of the adsorbed layer to be calculated. The polarization can be switched rapidly, allowing real-time measurements ofchemical reactions taking place on a chipsurface in a flow-through system. These measurements can be used to infer conformational information about themolecular interactions taking place, as the molecule size (from the layer thickness) and the fold density (from the RI) change. DPI is typically used to characterizebiochemical interactions by quantifying anyconformational change at the same time as measuring reaction rates, affinities and thermodynamics.[citation needed]

The technique is quantitative and real-time (10 Hz) with a dimensional resolution of 0.01 nm.[2]

Extensions of dual-polarization interferometry also exist, namely multiple pathlength dual-polarization interferometry (MPL-DPI)[3][4][5] and absorption enhanced DPI. In MPL-DPI quantification of both layer thickness and refractive index (density) and therefore mass per unit area can be made for in situ and ex-situ coated films, where normal DPI can only calculate film properties if the interferogram is constantly monitored. Absorption enhanced DPI[6] (AE-DPI) is used to separate the mass of different molecules on the surface, exploiting the absorption of one of the molecular species compared to the other species on the surface.

Applications

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A novel application for dual-polarization interferometry emerged in 2008, where the intensity of light passing through the waveguide is extinguished in the presence of crystal growth. This has allowed the very earliest stages in protein crystal nucleation to be monitored.[7] Later versions of dual-polarization interferometers also have the capability to quantify the order and disruption in birefringent thin films.[8] This has been used, for example, to study the formation of lipid bilayers and their interaction with membrane proteins.[9][10]

References

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  1. ^Cross, G; Reeves, AA; Brand, S; Popplewell, JF; Peel, LL; Swann, MJ; Freeman, NJ (2003). "A new quantitative optical biosensor for protein characterisation".Biosensors and Bioelectronics.19 (4):383–90.doi:10.1016/S0956-5663(03)00203-3.PMID 14615097.
  2. ^Swann, MJ; Freeman, NJ; Cross, GH (2007). "Dual Polarization Interferometry: A Real-Time Optical Technique for Measuring (Bio)Molecular Orientation, Structure and Function at the Solid/Liquid Interface". In Marks, R.S.; Lowe, C.R.; Cullen, D.C.; Weetall, H.H.; Karube, I. (eds.).Handbook of Biosensors and Biochips. Vol. 1.Wiley. Pt. 4, Ch. 33, pp. 549–568.ISBN 978-0-470-01905-4.
  3. ^Coffey, Paul D.; Swann, Marcus J.; Waigh, Thomas A.; Schedin, Fred; Lu, Jian R. (June 22, 2009)."Multiple path length dual polarization interferometry".Optics Express.17 (13):10959–10969.Bibcode:2009OExpr..1710959C.doi:10.1364/OE.17.010959.PMID 19550495.
  4. ^Coffey, Paul."Interfacial Measurements of Colloidal and Bio-colloidal Systems in Real-Time". RetrievedDecember 16, 2022.
  5. ^Delivopoulos, Evangelos; Ouberai, Myriam M.; Coffey, Paul D.; Swann, Marcus J.; Shakesheff, Kevin M.; Welland, Mark E. (February 2015)."Serum protein layers on parylene-C and silicon oxide: Effect on cell adhesion".Colloids and Surfaces B: Biointerfaces.126:169–177.doi:10.1016/j.colsurfb.2014.12.020.PMC 4342411.PMID 25555155.
  6. ^Coffey, Paul David; Swann, Marcus Jack; Waigh, Thomas Andrew; Mu, Qingshan; Lu, Jian Ren (2013). "The structure and mass of heterogeneous thin films measured with dual polarization interferometry and ellipsometry".RSC Advances.3 (10): 3316.Bibcode:2013RSCAd...3.3316C.doi:10.1039/C2RA22911K.
  7. ^Boudjemline, A; Clarke, DT; Freeman, NJ; Nicholson, JM; Jones, GR (2008). "Early stages of protein crystallization as revealed by emerging optical waveguide technology".Journal of Applied Crystallography.41 (3): 523.doi:10.1107/S0021889808005098.
  8. ^Mashaghi, A; Swann, M; Popplewell, J; Textor, M; Reimhult, E (2008). "Optical Anisotropy of Supported Lipid Structures Probed by Waveguide Spectroscopy and Its Application to Study of Supported Lipid Bilayer Formation Kinetics".Analytical Chemistry.80 (10):3666–76.doi:10.1021/ac800027s.PMID 18422336.
  9. ^Sanghera, N; Swann, MJ; Ronan, G; Pinheiro, TJ (2009)."Insight into early events in the aggregation of the prion protein on lipid membranes".Biochimica et Biophysica Acta (BBA) - Biomembranes.1788 (10):2245–51.doi:10.1016/j.bbamem.2009.08.005.PMID 19703409.
  10. ^Lee, TH; Heng, C; Swann, MJ; Gehman, JD; Separovic, F; Aguilar, MI (2010)."Real-time quantitative analysis of lipid disordering by aurein 1.2 during membrane adsorption, destabilisation and lysis".Biochimica et Biophysica Acta (BBA) - Biomembranes.1798 (10):1977–86.doi:10.1016/j.bbamem.2010.06.023.PMID 20599687.

Further reading

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Vibrational (IR)
UV–Vis–NIR "Optical"
X-ray and Gamma ray
Electron
Nucleon
Radiowave
Others
Data collection, processing
Measured phenomena
Applications
High resolution
Medium resolution
Spectroscopic
Translational diffusion
Rotational diffusion
Chemical
Thermodynamic
Computational
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