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US 6,643,300 B1Granted
Laser irradiation optical system
AssigneeMinolta Co., Ltd.
InventorYuichiro Ori
Life of this patent
Estimating the term…
Abstract
A laser irradiation optical system includes a dividing means for dividing a first entering laser beam once, and producing a plurality of second laser beams having beam widths equal to the beam which of the first laser beam and advancing in mutually different directions, a condensing means for condensing for condensing each second laser beam to mutually advance in near the same direction; and a shaping means for converting the intensity distribution of a cross section perpendicular to the optical path of each second laser beam in the optical paths of the mutually separated second laser beams.
Claims25
A laser irradiation optical system comprising:
- a dividing means for dividing a first entering laser beam once, and producing a plurality of second laser beams having beam widths equal to the beam width of the first laser beam and advancing in mutually different directions;
- a condensing means for condensing each second laser beam to mutually advance in nearly the same direction;
- and
- a shaping means for converting an intensity distribution of a cross section perpendicular to a system optical path in a laser optical path of each of the mutually separated second laser beams, the shaping means being arranged in the system optical path anterior to a focal plane where each second laser beam is condensed by the condensing means.
1 more element
A laser irradiation optical system comprising:
- a dividing means for dividing a first entering laser beam once, and producing a plurality of second laser beams having beam widths equal to the beam width of the first laser beam and advancing in mutually different directions;
- a condensing means for condensing each second laser beam to mutually advance in near the same direction;
- and
- a shaping means for converting the intensity distribution of a cross section perpendicular to a system optical path of each second laser beam in a laser optical path of each of the mutually separated second laser beams,
- wherein the dividing means is an element which divides a first laser beam by diffraction to produce a second laser beam;
- and
- wherein the condensing means is an element having a focal point on or near the dividing means, and arranged in the system optical path in a position where the second laser beams overlap;
- and which satisfies the relationship
- f·{1−m·λ·f/(p·W)}≦Zd≦f·{1+m·λ·f/(p·W)}
- where λ represents the wavelength of the first and second laser beams, f represents the focal length of the condensing means, m represents the minimum value of the absolute value of the difference of the degree of diffraction of the second laser beams in the same diffraction direction, W represents the beam width of the first laser beam in this diffraction direction, p represents the sequence period of the grating unit of the dividing means in this diffraction direction, and Zd represents the distance from the condensing means to the shaping means with the advancing direction of the second laser beam designated positive.
7 more elements
A laser irradiation optical system comprising:
- a dividing means for dividing a first entering laser beam once, and producing a plurality of second laser beams having beam widths equal to the beam width of the first laser beam and advancing in mutually different directions;
- a condensing means for condensing each second laser beam to mutually advance in near the same direction;
- and
- a shaping means for converting an intensity distribution of a cross section perpendicular to a system optical path of each second laser beam in a laser optical path of each of the mutually separated second laser beams,
- wherein the dividing means is an element which divides a first laser beam by diffraction to produce a second laser beam;
- and
- wherein the condensing means is an element having a focal point on or near the dividing means, and arranged in the system optical path in a position where the second laser beams do not overlap;
- and which satisfies the relationship
- f·{p·W/(m·λ·f)−1}≦Zd≦f·{1+m·λ·f/(p·W)}
- where λ represents the wavelength of the first and second laser beams, f represents the focal length of the condensing means, m represents the minimum value of the absolute value of the difference of the degree of diffraction of the second laser beams in the same diffraction direction, W represents the beam width of the first laser beam in this diffraction direction, p represents the sequence period of the grating unit of the dividing means in this diffraction direction, and Zd represents the distance from the condensing means to the shaping means with the advancing direction of the second laser beam designated positive.
7 more elements
A method of converting a laser beam comprising the steps of:
- dividing the laser beam into a plurality of diverging secondary laser beams, each secondary laser beam having a beam width approximately equal to the beam width of the laser beam;
- condensing each of the plurality of secondary laser beams such that each of the thus condensing secondary laser beams are directed in nearly the same direction;
- and
- altering an intensity distribution of a cross section of a respective secondary laser optical path of each secondary laser beam, each cross section being perpendicular to a system optical path and being in a position anterior to a focal plane where each secondary laser beam is condensed by the condensing means.
1 more element
A laser irradiation optical system comprising:
- a divider that divides a first entering laser beam once, and produces a plurality of second laser beams having beam widths equal to the beam width of the first laser beam and advancing in mutually different directions;
- a condenser that condenses each second laser beam to mutually advance in nearly the same direction;
- and
- a shaper that converts an intensity distribution of a cross section perpendicular to a system optical path in a laser optical path of each of the mutually separated second laser beams, the shaper being arranged in the system optical path anterior to a focal plane where each second laser beam is condensed by the condenser.
1 more element
A laser irradiation optical system comprising:
- a divider that divides a first entering laser beam once, and produces a plurality of second laser beams having beam widths equal to the beam width of the first laser beam and advancing in mutually different directions;
- a condenser that condenses each second laser beam to mutually advance in near the same direction;
- and
- a shaper that converts the intensity distribution of a cross section perpendicular to a system optical path of each second laser beam in a laser optical path of each of the mutually separated second laser beams,
- wherein the divider is an element which divides a first laser beam by diffraction to produce a second laser beam;
- and
- wherein the condenser is an element having a focal point on or near the divider, and is arranged in the system optical path in a position where the second laser beams overlap;
- and which satisfies the relationship
- f·{1−m·λ·f/(p·W)}≦Zd≦f·{1+m·λ·f/(p·W)}
- where λ represents the wavelength of the first and second laser beams, f represents the focal length of the condenser, m represents the minimum value of the absolute value of the difference of the degree of diffraction of the second laser beams in the same diffraction direction, W represents the beam width of the first laser beam in this diffraction direction, p represents the sequence period of the grating unit of the divider in this diffraction direction, and Zd represents the distance from the condenser to the shaper with the advancing direction of the second laser beam designated positive.
7 more elements
A laser irradiation optical system comprising:
- a divider that divides a first entering laser beam once, and produces a plurality of second laser beams having beam widths equal to the beam width of the first laser beam and advancing in mutually different directions;
- a condenser that condenses each second laser beam to mutually advance in near the same direction;
- and
- a shaper that converts the intensity distribution of a cross section perpendicular to a system optical path of each second laser beam in a laser optical path of each of the mutually separated second laser beams,
- wherein the divider is an element which divides a first laser beam by diffraction to produce a second laser beam;
- and
- wherein the condenser is an element having a focal point on or near the divider, and arranged in the system optical path in a position where the second laser beams do not overlap;
- and which satisfies the relationship
- f·{p·W/(m·λ·f)−1}≦Zd≦f·{1+m·λ·f/(p·W)}
- where λ represents the wavelength of the first and second laser beams, f represents the focal length of the condenser, m represents the minimum value of the absolute value of the difference of the degree of diffraction of the second laser beams in the same diffraction direction, W represents the beam width of the first laser beam in this diffraction direction, p represents the sequence period of the grating unit of the divider in this diffraction direction, and Zd represents the distance from the condenser to the shaper with the advancing direction of the second laser beam designated positive.
7 more elements
Dependencies are inferred from the claim text.