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Описание презентации Metal-Insulator-Semiconductor and Metal-Insulator-Metal Structures. Part II. по слайдам
Metal-Insulator-Semiconductor and Metal-Insulator-Metal Structures. Part II. Heterogeneous Structures. Diodes Alexander Gabovich , KPI , Lecture
Transport properties of semiconductors
Transport properties of semiconductors
Transport properties of semiconductors
Transport properties of semiconductors
Transport properties of semiconductors
Transport properties of semiconductors
Transport properties of semiconductors
Transport properties of semiconductors
Transport properties of semiconductors
Transport properties of semiconductors
Transport properties of semiconductors
Transport properties of semiconductors
The PN junction diode
The PN junction diode
The PN junction diode
The PN junction diode
The PN junction diode
The PN junction diode
The PN junction diode
The PN junction diode
The PN junction diode
The PN junction diode
The PN junction diode Actually, the electromagnetic induction D rather than the field E should be continuous. However, here it does not matter because the dielectric constant ε is the same in the whole area.
The PN junction diode
The PN junction diode
The PN junction diode
The PN junction diode. Biased junction
The PN junction diode. Biased junction
The PN junction diode. Biased junction
The PN junction diode. Biased junction
The PN junction diode. Biased junction
The PN junction diode. Biased junction
The PN junction diode. Solar cell
The PN junction diode. Solar cell