Defect inspection apparatus and defect inspection method
View Patent ↗Method for realizing an inspection with short wavelength, high power light source and large numerical aperture, high performance optics to improve defect inspection sensitivity is disclosed. Short wavelength high power laser is realized by using a pulse oscillation type laser suitable for generation of high output power in a short-wavelength region. In addition, a spectral bandwidth of the laser is narrowed down so that amount of chromatic aberration of detection optics with single glass material (i.e. without compensation of chromatic aberration) is lowered to permissible level. Using highly workable glass material to construct the detection optics enables necessary surface accuracy or profile irregularity conditions to be met, even if the number of lenses is increased for large NA or the lens doesn't have a rotationally symmetrical aperture.
1. A defect inspection apparatus comprising:
a pulsed laser light source for emitting ultraviolet light;
illumination optics for irradiating with the light a surface of a sample;
first detection optics for forming a first enlarged image of the surface of the sample;
an image sensor for detecting light scattered on the sample to acquire the first enlarged image of the sample; and
an image processing unit for processing the first enlarged image of the sample;
wherein:
the pulsed laser light source comprises:
a semiconductor laser as an oscillator;
a signal source for generating pulse signals for driving the semiconductor laser;
an amplifier disposed posterior to the semiconductor laser; and
a wavelength converter configured to convert light amplified by the amplifier into the ultraviolet light,
a spectral bandwidth of the semiconductor laser is controlled by changing a pulse length of each of the pulse signals, and
a spectral bandwidth of the ultraviolet light emitted from the pulsed laser light source falls within a light-spectral bandwidth range permissible according to a particular chromatic aberration level of the illumination optics and a particular chromatic aberration level of the first detection optics.
2. The defect inspection apparatus according to claim 1 , wherein:
a spectral bandwidth of the ultraviolet light emitted from the pulsed laser light source is between 10 pm to 20 pm.
3. The defect inspection apparatus according to claim 1 , wherein:
a spectral bandwidth of a light emitted from the semiconductor laser is between 40 pm to 100 pm and the wave length converter converts the light emitted from the semiconductor laser into an ultraviolet light having spectral bandwidth between 10 pm to 20 pm.
4. A defect inspection apparatus comprising:
a pulsed laser light source for emitting ultraviolet light;
illumination optics for irradiating with the light a surface of a sample;
first detection optics for forming a first enlarged image of the surface of the sample;
an image sensor for detecting light scattered on the sample to acquire the first enlarged image of the sample; and
an image processing unit for processing the first enlarged image of the sample;
wherein:
the pulsed laser light source comprises:
a semiconductor laser as an oscillator;
a signal source for generating pulse signals for driving the semiconductor laser;
an amplifier disposed posterior to the semiconductor laser; and
a wavelength converter configured to convert light amplified by the amplifier into the ultraviolet light,
a spectral bandwidth of the semiconductor laser is controlled by changing a pulse length of each of the pulse signals,
a spectral bandwidth of the ultraviolet light emitted from the pulsed laser light source falls within a light-spectral bandwidth range permissible according to a particular chromatic aberration level of the illumination optics and a particular chromatic aberration level of the first detection optics, and
an offset current exceeding a threshold level is supplied to the semiconductor laser as a driving current during a pulse-to-pulse period to maintain laser oscillation.
5. A defect inspection method comprising the steps of:
emitting ultraviolet light from a pulsed laser light source;
irradiating the light to a surface of a sample;
forming a first enlarged image of the surface of the sample;
detecting light scattered on the sample to acquire the first enlarged image of the sample; and
processing the first enlarged image of the sample;
wherein:
the pulsed laser light source comprises:
a semiconductor laser as an oscillator;
a signal source for generating pulse signals for driving the semiconductor laser;
an amplifier disposed posterior to the semiconductor laser; and
a wavelength converter configured to convert light amplified by the amplifier into the ultraviolet light,
a spectral bandwidth of the semiconductor laser is controlled by changing a pulse length of each of the pulse signals, and
a spectral bandwidth of the ultraviolet light emitted from the pulsed laser light source falls within a light-spectral bandwidth range permissible according to a particular chromatic aberration level of an illumination optics for irradiating the ultraviolet light and a particular chromatic aberration level of a first detection optics for forming the first enlarged image.
6. The defect inspection method according to claim 5 , wherein:
a spectral bandwidth of the ultraviolet light emitted from the pulsed laser light source is between 10 pm to 20 pm.
7. The defect inspection method according to claim 5 , wherein:
a spectral bandwidth of a light emitted from the semiconductor laser is between 40 pm to 100 pm and the wave length converter converts the light emitted from the semiconductor laser into an ultraviolet light having spectral bandwidth between 10 pm to 20 pm.
8. The defect inspection method according to claim 5 , wherein:
an offset current exceeding a threshold level is supplied to the semiconductor laser as a driving current during a pulse-to-pulse period to maintain laser oscillation.
9. A pulsed laser light source comprising:
a semiconductor laser as an oscillator;
a signal source for generating pulse signals for driving the semiconductor laser;
an amplifier disposed posterior to the semiconductor laser; and
a wavelength converter configured to convert light amplified by the amplifier into ultraviolet light,
wherein a spectral bandwidth of the semiconductor laser is controlled by changing a pulse length of each of the pulse signals, and
a spectral bandwidth of the ultraviolet light falls within a light-spectral bandwidth range permissible according to a particular chromatic aberration level of illumination optics irradiating the ultraviolet light and a particular chromatic aberration level of first detection optics forming a first enlarged image of a sample.
10. The pulsed laser light source according to claim 9 , wherein:
a spectral bandwidth of the ultraviolet light is between 10 pm to 20 pm.
11. The pulsed laser light source according to claim 9 , wherein:
a spectral bandwidth of a light emitted from the semiconductor laser is between 40 pm to 100 pm and the wave length converter converts the light emitted from the semiconductor laser into an ultraviolet light having spectral bandwidth between 10 pm to 20 pm.
12. A pulsed laser light source comprising:
a semiconductor laser as an oscillator;
a signal source for generating pulse signals for driving the semiconductor laser;
an amplifier disposed posterior to the semiconductor laser; and
a wavelength converter configured to convert light amplified by the amplifier into ultraviolet light,
wherein a spectral bandwidth of the semiconductor laser is controlled by changing a pulse length of each of the pulse signals,
a spectral bandwidth of the ultraviolet light falls within a light-spectral bandwidth of the ultraviolet light falls within a light-spectral bandwidth range permissible according to a particular chromatic aberration level of illumination optics irradiating the ultraviolet light and a particular chromatic aberration level of first detection optics forming a first enlarged image of a sample,
an offset current exceeding a threshold level is supplied to the semiconductor laser as a driving current during a pulse-to-pulse period to maintain laser oscillation.