APPARATUS FOR INSPECTING SURFACE OF OBJECT

In semiconductor inspection using second-harmonic generation within an object, a weak second-harmonic is detected at high sensitivity. In a semiconductor inspecting apparatus which irradiates a pulsed laser with a very short pulse width to a surface of a semiconductor device as the object, and measu...

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Bibliographische Detailangaben
Hauptverfasser:	HIDAKA, YASUHIRO, KIM, INGI
Format:	Patent
Sprache:	eng
Schlagworte:	BASIC ELECTRIC ELEMENTS DEVICES OR ARRANGEMENTS, THE OPTICAL OPERATION OF WHICH ISMODIFIED BY CHANGING THE OPTICAL PROPERTIES OF THE MEDIUM OF THEDEVICES OR ARRANGEMENTS FOR THE CONTROL OF THE INTENSITY,COLOUR, PHASE, POLARISATION OR DIRECTION OF LIGHT, e.g.SWITCHING, GATING, MODULATING OR DEMODULATING ELECTRIC SOLID STATE DEVICES NOT OTHERWISE PROVIDED FOR ELECTRICITY FREQUENCY-CHANGING INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIRCHEMICAL OR PHYSICAL PROPERTIES MEASURING NON-LINEAR OPTICS OPTICAL ANALOGUE/DIGITAL CONVERTERS OPTICAL LOGIC ELEMENTS OPTICS PHYSICS SEMICONDUCTOR DEVICES TECHNIQUES OR PROCEDURES FOR THE OPERATION THEREOF TESTING
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Beschreibung
Zusammenfassung:	In semiconductor inspection using second-harmonic generation within an object, a weak second-harmonic is detected at high sensitivity. In a semiconductor inspecting apparatus which irradiates a pulsed laser with a very short pulse width to a surface of a semiconductor device as the object, and measures the second-harmonic generated within the semiconductor device, a second-harmonic generation element is disposed between a light source and the object to generate a first second-harmonic. Further, the apparatus modulates a phase of only the first second-harmonic using an electric optical crystal, and then, a fundamental wave is irradiated onto the object. When the fundamental wave is irradiated onto the semiconductor device, the second-harmonic is generated therefrom. The first second-harmonic interferes with the second second-harmonic on a detector, and an intensity of the light obtained by the interfering is modulated at the same period as that of the phase modulation of the first second-harmonic. An amplitude of the second second-harmonic may be obtained from a modulated amplitude thereof, and a phase of the second second-harmonic may be measured from a modulated phase thereof.