IP Library Granted Patent US 10,288,412
Granted Patent B2
US 10,288,412 · App. 15/996,941 · Granted May 14, 2019

Optical measurement apparatus and optical measurement method

Inventors: Nobuyuki Inoue (Kyoto, JP); Kunikazu Taguchi (Hirakata, JP)
Assignee: Otsuka Electronics Co., Ltd.
G01B11/06G01B9/02024G01B9/02041G01B9/02043
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Quick Facts
Patent No.
US 10,288,412
App. No.
15/996,941
Granted
May 14, 2019
Kind
B2
Abstract

An optical measurement apparatus includes an irradiation optical system which linearly irradiates a measurement target with measurement light having a certain wavelength range, a measurement optical system which receives linear measurement interference light which is transmitted light or reflected light originating from the measurement target as a result of irradiation with the measurement light, and a processing device. The processing device includes a first calculation module that calculates a modification factor depending on with an angle of incidence on the measurement optical system from each measurement point in association with a region in the two-dimensional image corresponding to each measurement point in the measurement target irradiated with the measurement light and a second calculation module that calculates optical characteristics of the measurement target by applying the corresponding modification factor to a value for each pixel included in the two-dimensional image.

Claims (45)

1. An optical measurement apparatus comprising:

an irradiation optical system configured to linearly irradiate a measurement target with measurement light having a certain wavelength range;

a measurement optical system which receives linear measurement interference light which is transmitted light or reflected light originating from the measurement target as a result of irradiation with the measurement light; and

a processing device, wherein

the measurement optical system comprises

a diffraction grating which expands the measurement interference light in a wavelength direction orthogonal to a longitudinal direction of the measurement interference light, and

an imaging portion which outputs a two-dimensional image by receiving the measurement interference light expanded in the wavelength direction by the diffraction grating, and

the processing device comprises

a first calculation module that calculates a modification factor depending on an angle of incidence on the measurement optical system from each measurement point in association with a region in the two-dimensional image corresponding to each measurement point in the measurement target irradiated with the measurement light, and

a second calculation module that calculates optical characteristics of the measurement target by applying a corresponding modification factor to each pixel value included in the two-dimensional image.

2. The optical measurement apparatus according to claim 1 , wherein

the modification factor includes a wave number representing a parameter including a wavelength of the measurement light and a refractive index of the measurement target, and

the wave number is calculated in consideration of magnitude of a corresponding angle of incidence, for each pixel position in the two-dimensional image.

3. The optical measurement apparatus according to claim 2 , wherein

the second calculation module is configured to

subject a row of values resulting from conversion in accordance with a relational expression for linearizing the pixel value in the two-dimensional image corresponding to a measurement point of interest with respect to a phase factor, to Fourier transform with respect to a row of corresponding wave numbers,

determine a film thickness at the measurement point of interest based on a peak position which appears in a power spectrum obtained through the Fourier transform, and

aggregate film thicknesses determined for a plurality of the measurement points and outputting a resultant aggregate as a film thickness distribution.

4. The optical measurement apparatus according to claim 2 , wherein

the wave number is calculated in consideration of wavelength-dependency of a refractive index of the measurement target.

5. The optical measurement apparatus according to claim 1 , wherein

the modification factor includes a value representing magnitude of an angle of incidence corresponding to each measurement point, and

the second calculation module is configured to

adopt a film thickness at each measurement point as a fluctuating parameter and calculate a theoretical value of each pixel corresponding to the two-dimensional image based on a refractive index of the measurement target, a value representing magnitude of the angle of incidence corresponding to each measurement point, and correspondence between each measurement point and a pixel position in the two-dimensional image, and

determine a film thickness at each measurement point by adjusting the fluctuating parameter such that a similarity between the calculated theoretical value of each pixel and each pixel value of the two-dimensional image is higher.

6. An optical measurement method comprising:

linearly irradiating a measurement target with measurement light having a certain wavelength range and receiving linear measurement interference light which is transmitted light or reflected light originating from the measurement target as a result of irradiation with the measurement light;

expanding the measurement interference light in a wavelength direction orthogonal to a longitudinal direction of the measurement interference light and outputting a two-dimensional image by receiving the measurement interference light expanded in the wavelength direction;

calculating a modification factor depending on an angle of incidence from each measurement point in association with a region in the two-dimensional image corresponding to each measurement point in the measurement target irradiated with the measurement light; and

calculating optical characteristics of the measurement target by applying a corresponding modification factor to each pixel value included in the two-dimensional image.

7. The optical measurement method according to claim 6 , wherein

the modification factor includes a wave number representing a parameter including a wavelength of the measurement light and a refractive index of the measurement target, and

the wave number is calculated in consideration of magnitude of a corresponding angle of incidence, for each pixel position in the two-dimensional image.

8. The optical measurement method according to claim 7 , wherein

the calculating optical characteristics includes

subjecting a row of values resulting from conversion in accordance with a relational expression for linearizing the pixel value of the two-dimensional image corresponding to a measurement point of interest with respect to a phase factor, to Fourier transform with respect to a row of corresponding wave numbers,

determining a film thickness at the measurement point of interest based on a peak position which appears in a power spectrum obtained through the Fourier transform, and

aggregating film thicknesses determined for a plurality of the measurement points and outputting a resultant aggregate as a film thickness distribution.

9. The optical measurement method according to claim 7 , wherein

the wave number is calculated in consideration of wavelength-dependency of a refractive index of the measurement target.

10. The optical measurement method according to claim 6 , wherein

the modification factor includes a value representing magnitude of an angle of incidence corresponding to each measurement point, and

the calculating optical characteristics includes

adopting a film thickness at each measurement point as a fluctuating parameter and calculating a theoretical value of each pixel corresponding to the two-dimensional image based on a refractive index of the measurement target, a value representing magnitude of the angle of incidence corresponding to each measurement point, and correspondence between each measurement point and a pixel position in the two-dimensional image, and

determining a film thickness at each measurement point by adjusting the fluctuating parameter such that a similarity between the calculated theoretical value of each pixel and each pixel value of the two-dimensional image is higher.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Jun 4, 2018
From: INOUE, NOBUYUKI; TAGUCHI, KUNIKAZU
To: OTSUKA ELECTRONICS CO., LTD.
Reel/Frame 045978/0733 →
Priority Claims (1)
JP 2017-111043 · Jun 5, 2017 · national
Continuity (1)
Related Publication 20180347964A1 · Dec 6, 2018
Cited By (1)
US 12,442,774