Abstract
You should know about ice that may melt under sunlight and changes to water. The water can further change to vapor by heating. They form three common states of mater around the world, that is, the solid, liquid and gas. Nevertheless, do you know what may happen when a gas is further heated to an extremely high temperature such as that in the sun? Science tells us that the gas there will not be stable any more but immediately collapse. The electrons escape from the atomic orbits to become free, leaving behind the bare atoms as positively charged particles. The sun is thus full of negatively charged electrons and positively charged ions but they exist as a spherical whole. That is called plasma, the fourth state of matter, in addition to the solid, liquid and gaseous states.
Access this chapter
Tax calculation will be finalised at checkout
Purchases are for personal use only
References
Sturrock PA (1994) Plasma physics: an introduction to the theory of astrophysical. Geophysical and laboratory plasmas. Cambridge University Press, Cambridge
Hazeltine RD, Waelbroeck FL (2004) The framework of plasma physics. Westview Press, Boulder
Chen FF (2006) Introduction to plasma physics and controlled fusion. Springer, New York
Crookes W (1879) On radiant matter; a lecture delivered to the British Association for the Advancement of Science, at Sheffield, Friday, August 22, 1879. Am J Sci 318(106):241–262
Preston S (1881) On some points relating to the dynamics of “Radiant Matter.” Nature 23:461–464. https://doi.org/10.1038/023461a0
Thomson JJXL (1897) Cathode Rays. London Edinburgh Dublin Philos Mag J Sci 44:293–316. https://doi.org/10.1080/14786449708621070
Langmuir I (1928) Oscillations in ionized gases. PNAS 14:627–637. https://doi.org/10.1073/pnas.14.8.627
Goldston RJ, Rutherford PH (1995) Introduction to plasma physics. Taylor & Francis, New York, pp 1–2
Pines D, Bohm D (1952) A collective description of electron interactions: II. Collective vs individual particle aspects of the interactions. Phys Rev 85:338–353
Ritchie RH (1957) Plasma losses by fast electrons in thin films. Phys Rev 106:874–881
Bohm D, Pines D (1953) A collective description of electron interactions: III. Coulomb interactions in a degenerate electron gas. Phys Rev 92:609–625. https://doi.org/10.1103/physrev.92.609
Stern EA, Ferrell RA (1960) Surface plasma oscillations of a degenerate electron gas. Phys Rev 120:130–136
Zeng S, Yu X, Law W-C, Zhang Y, Hu R, Dinh X-Q, Ho H-P, Yong K-T (2013) Size dependence of Au NP-enhanced surface plasmon resonance based on differential phase measurement. Sens Actuat B Chem 176:1128–1133. https://doi.org/10.1016/j.snb.2012.09.073
Raether H (1988) Surface plasmons on smooth and rough surfaces and on gratings. Springer, New York
Harsh OK, Agarwal BK (1988) Surface plasmon dispersion relation in the X-ray emission spectra of a semi-infinite rectangular metal bounded by a plane. Phys B+C 150:378–384. https://doi.org/10.1016/0378-4363(88)90078-2
Wood RW (1902) On a remarkable case of uneven distribution of light in a diffraction grating spectrum. Phil Mag 4:396–402
Wood RW (1902) A suspected case of the electrical resonance of minute metal particles for light-waves. A new type of absorption. Proc Phys Soc Lond 18:1478
Chen CY, Chang CC, Yu C, Lin CW (2012) Clinical application of surface plasmon resonance-based biosensors for fetal fibronectin detection. Sensors 12:3879–3890
Fei Z, Rodin AS, Andreev GO, Bao W, McLeod AS, Wagner M, Zhang LM, Zhao Z, Thiemens M, Dominguez G, Fogler MM, Castro Neto AH, Lau CN, Keilmann F, Basov DN (2012) Gate-tuning of graphene plasmons revealed by infrared nano-imaging. Nature 487:82–85. https://doi.org/10.1038/nature11253
Yan H, Low T, Zhu W, Wu Y, Freitag M, Li X, Guinea F, Avouris P, Xia F (2013) Damping pathways of mid-infrared plasmons in graphene nanostructures. Nat Photonics 7:394–399. https://doi.org/10.1038/nphoton.2013.57
Maxwell-Garnett JC (1904) Colors in metal glasses and in metallic film. Philos Trans R Soc London 203:385–420
Drude P (1900) Zur Elektronentheorie der metalle. Ann Phys 306(3):566–613. https://doi.org/10.1002/andp.19003060312
Rayleight L (1907) Note on the remarkable case of diffraction spectra described by Prof. Wood. Phil Mag 14:60–65
Mie G (1908) Beiträge zur Optik trüber Medien, speziell kolloidaler Metallösungen. Ann Phys 25:377–455
Fano U (1941) The theory of anomalous diffraction gratings and of quasi-stationary waves on metallic surfaces (Sommerfeld’s waves). J Opt Soc Am 31:213–222
Sommerfeld A (1899) Über die Fortpflanzung elektrodynamischer Wellen an längs eines Drahtes. Ann der Physik und Chemie 302(2):233–290
Zenneck J (1907) Über die Fortpflanzung ebener elektromagnetischer Wellen längs einer ebenen Leiterfläche und ihre Beziehung zur drahtlosen Telegraphie. Ann der Physik 23:846–866
Pines D (1956) Collective energy losses in solid. Rev Mod Phys 28:184–198
Fano U (1956) Atomic theory of electromagnetic interactions in dense materials. Phys Rev 103:1202–1218
Powell CJ, Swan JB (1959) Origin of the characteristic electron energy losses in aluminum. Phys Rev 115:869–875
Powell CJ, Swan JB (1960) Effect of oxidation on the characteristic loss spectra of aluminum and magnesium. Phys Rev 118:640–643
Ritchie RH, Arakawa ET, Cowan JJ, Hamm RH (1968) Surface-plasmaon resonance effect in grating diffraction. Phys Rev Lett 21:1530–1532
Kreibig U, Zacharias P (1970) Surface plasma resonances in small spherical silver and gold particles. Z Phys 231:128–143
Cunningham SL, Maradudin AA, Wallis RF (1974) Effect of a charge layer on the surface-plasmon-polarization dispersion curve. Phys Rev B 10:3342–3355
Fleschmann M, Hendra PJ, McQuillan AJ (1974) Raman spectra of pyridine adsorbed at a silver electrode. Chem Phys Lett 26:163–166
Zia R, Schuller JA, Brongers ML (2006) Plasmonics: the next chip-scale technology. Mater Today 9:20–27
Otto A (1968) Excitation of nonradiative surface plasma waves in silver by the method of frustrated total reflection. Z Phys A Hadrons Nucl 216:398–410
Kretschmann E, Raether H (1968) Radiative decay of non-radiative surface plasmons excited by light. Z Naturf 23A:2135–2136
Kretschmann E (1971) Die bestimmung optischer konstanten von metallen durch anregung von oberfliichenplasmaschwingungen. Z Phys 241:313–324
Owen V (1997) Real-time optical immunosensors-A commercial reality. Biosens Bioelect 12:i–ii
Gordon JG II, Swalen JD (1977) The effect of thin organic films on the surface plasma resonance on gold. Opt Commun 22(3):374–376
Gordon JG II, Ernst S (1980) Surface plasmons as a probe of the electrochemical interface. Surf Sci 101(1–3):499–506
Nylander C, Liedberg B, Lind T (1982–1983) Gas detection by means of surface plasmon resonance. Sens Actuat 3:79–88
Liedberg B, Nylander C, Lunström I (1983) Surface plasmon resonance for gas detection and biosensing. Sens Actuat 4:299–304
Rycenga M, Cobley CM, Zeng J, Li W, Moran CH, Zhang Q, Qin D, Xia Y (2011) Controlling the synthesis and assembly of silver nanostructures for plasmonic applications. Chem Rev 111:3669–3712
Liu X, Swihart MT (2014) Heavily-doped colloidal semiconductor and metal oxide nanocrystals: an emerging new class of plasmonic nanomaterials. Chem Soc Rev 43:3908–3920
Toma K, Vala M, Adam P, Homola J, Knoll W, Dostálek J (2013) Compact surface plasmon-enhanced fluorescence biochip. Opt Express 21:10121–10132
Bao W, Staffaroni M, Bokor J, Salmeron MB, Yablonovitch E, Cabrini S, Bargioni AW, Schuck PJ (2013) Plasmonic near-field probes: a comparison of the campanile geometry with other sharp tips. Opt Exp 21:8166–8176
Yeatman E, Ash EA (1987) Surface plasmon microscopy. Elect Lett 23:1091–1092
Rothenhäuslar B, Knoll W (1988) Surface plasmon microscopy. Nature 332:615–617
Roberta DA, Spoto G (2013) Surface plasmon resonance imaging for nucleic acid detection. Anal Bioanal Chem 405:573–584
Wark AW, Lee HJ, Corn RM (2005) Long-range surface plasmon resonance imaging for bioaffinity sensors. Anal Chem 77:3904–3907
Sarid D (1981) Long-range surface-plasma waves on very thin metal films. Phys Rev Lett 47:1927–1930
Quail JC, Rako JG, Simon HJ (1983) Long-range surface-plasmon modes in silver and aluminum films. Opt Lett 8:377–379
Matsubara K, Kawata S, Minami S (1990) Multilayer system for a high-precision surface plasmon resonance sensor. Opt Lett 15:75–77. https://doi.org/10.1364/OL.15.000075
Yang F, Bradberry GW, Sambles JR (1991) Long-range surface mode supported by very thin silver films. Phys Rev Lett 66:2030–2032
Kessler MA, Hall EAH (1996) Multilayered structures exhibiting long-range surface exciton resonance. Thin Solid Films 272:161–169
Lyndin NM, Salakhutdinov IF, Sychugov VA, Usievich BA, Pudonin FA, Parriaux O (1999) Long-range surface plasmons in asymmetric layered metal-dielectric structures. Sens Actuat B 54:37–42
Shumaker-Parry JS, Campbell CT (2004) Quantitative methods for spatially resolved adsorption/ desorption measurements in real time by surface plasmon resonance microscopy. Anal Chem 76:907–917
Johansen K (2005) Imaging SPR apparatus. U.S. patent 6862094, March 1, 2005
Axelrod D (2001) Total internal reflection fluorescence microscopy in cell biology. Traffic 2:764–774
Huang B, Yu F, Zare RN (2007) Surface plasmon resonance imaging using a high numerical aperture microscope objective. Anal Chem 79:2979–2983
Author information
Authors and Affiliations
Corresponding author
Rights and permissions
Copyright information
© 2023 Springer Nature Singapore Pte Ltd.
About this chapter
Cite this chapter
Chen, Y. (2023). Introduction. In: Surface Plasmon Resonance Imaging. Lecture Notes in Chemistry, vol 95. Springer, Singapore. https://doi.org/10.1007/978-981-99-3118-7_1
Download citation
DOI: https://doi.org/10.1007/978-981-99-3118-7_1
Published:
Publisher Name: Springer, Singapore
Print ISBN: 978-981-99-3117-0
Online ISBN: 978-981-99-3118-7
eBook Packages: Chemistry and Materials ScienceChemistry and Material Science (R0)