[1]
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E. A. Anagnostakis, “Characterisation of Semiconductor Epitaxial Layer Interfaces by Persistent Photoconductivity,” Physica Status Solidi A, Vol. 126, No. 2, 1991, pp. 397-410. doi:10.1002/pssa.2211260211
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[2]
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E. A. Anagnostakis, “Photoconductive Gain of Semiconductor Epitaxial Layers,” Physica Status Solidi A, Vol. 127, No. 1, 1991, pp. 153-158.
doi:10.1002/pssa.2211270116
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[3]
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D. E. Theodorou and E. A. Anagnostakis, “Persistent Photoconductivity and DX Centres,” Physical Review B, Vol. 44, 1991, pp. 352-3354.
doi:10.1103/PhysRevB.44.3352
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[4]
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E. A. Anagnostakis, “Photoconductive Response of GaAs Epitaxial Layers,” Applied Physics A, Vol. 54, No. 1, 1992, pp. 68-71. doi:10.1007/BF00348133
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[5]
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E. A. Anagnostakis, “Proposition of an Effective Wave Function for the 2DEG within MODFET Heterostructures,” Physica Status Soilidi B, Vol. 171, No. 2, 1992, pp. K75-K78. doi:10.1002/pssb.2221710226
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[6]
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E. A. Anagnostakis, “Lateral Photovoltage as a Probe of MODFET Channel Disorder,” Physica Status Solidi B, Vol. 172, 1992, pp. K61-K63.
doi:10.1002/pssb.2221720228
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[7]
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E. A. Anagnostakis, “Determination of Persistent Photoconductivity within Semiconductor Epitaxial Layers by Photoconductive Gain,” Physical Review B, Vol. 46, No. 12, 1992, pp. 7593-7595. doi:10.1103/PhysRevB.46.7593
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[8]
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E. A. Anagnostakis and D. E. Theodorou, “Determination of Two Dimensional Electron Gas Population Enhancement within Illuminated Semiconductor Heterostructures by Persistent Photoconductivity,” Journal of Applied Physics, Vol. 73, No. 9, 1993, pp. 4550-4554.
doi:10.1063/1.352800
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[9]
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E. A. Anagnostakis, “Negative Differential Mobility Features in the Persistent Photoconductive Response of Semiconductor Devices,” Physica Status Solidi A, Vol. 136, No. 1, 1993, pp. 247-250.
doi:10.1002/pssa.2211360131
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[10]
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E. A. Anagnostakis, “On a Generic Equation Modelling the Persistent Photoconductive Response of Semiconductor Devices,” Physica Status Solidi B, Vol. 177, No. 2, 1993, pp. 533-536. doi:10.1002/pssb.2221770230
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[11]
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E. A. Anagnostakis, “Designing a Launcher-Receptor Quantum Electron Device,” Physica Status Solidi B, Vol. 181, No. 1, 1994, pp. K15-K17.
doi:10.1002/pssb.2221810127
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[12]
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E. A. Anagnostakis, “Quantum Well Character of Semiconductor Homostructures Underlying the Occurrence of a Negative Differential Mobility,” Physica Status Solidi A, Vol. 141, No. 2, 1994, pp. 373-379.
doi:10.1002/pssa.2211410216
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[13]
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E. A. Anagnostakis, “Photoconductive Studies of Carrier Mobility across Semiconductor Surface Depletion Zones,” Physica Status Solidi A, Vol. 146, No. 2, 1994, pp. K9- K11. doi:10.1002/pssa.2211460236
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[14]
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E. A. Anagnostakis and D. E. Theodorou, “Semiconductor Heterointerface Characterisation via Effective Harmonic Oscillator Simulation,” Physica Status Solidi B, Vol. 188, No. 2, 1995, pp. 689-695.
doi:10.1002/pssb.2221880212
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[15]
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E. A. Anagnostakis, “Nanoheterointerface Wave Function Penetration Length Photonic Characterization,” Reviews on Advanced Materials Science, Vol. 12, No. 2, 2006, pp. 182-188.
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[16]
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E. A. Anagnostakis, “Semiconductor-Nanoheterointerface Eigenstate Photonic Modification”, Journal of Non-Cry- stalline Solids, Vol. 354, No. 1, 2008, pp. 4233-4237.
doi:10.1016/j.jnoncrysol.2008.06.029
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[17]
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E. A. Anagnostakis, “Responsivity Robustness of Radio- ctivity-Irradiated Nanosensors,” WSEAS Transactions on Circuits and Systems, Vol. 8, No. 3, 2009, pp. 311-320.
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[18]
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E. A. Anagnostakis, “On a Scheme of Nanoheterointerfacial Intersubband 15-THz Luminescence,” Physica B, Vol. 405, No. 1, 2010, pp. 25-28.
doi:10.1016/j.physb.2009.08.010
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[19]
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E. A. Anagnostakis, “Optoelectronic Nanoheterointerface Functional Eigenstate Photodynamics,” Physica B, Vol. 405, No. 1, 2010, pp. 38-40.
doi:10.1016/j.physb.2009.08.002
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[20]
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E. A. Anagnostakis, “Quantum-Well Tridiagonal: A Qua- litative Comprehension of Optoelectronics Nanotechnology,” WSEAS Transactions on Circuits and Systems, Vol. 9, No. 1, 2010, pp. 1-10.
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