US20100254020A1 - Laser line generator - Google Patents

Laser line generator Download PDF

Info

Publication number
US20100254020A1
US20100254020A1 US12/418,710 US41871009A US2010254020A1 US 20100254020 A1 US20100254020 A1 US 20100254020A1 US 41871009 A US41871009 A US 41871009A US 2010254020 A1 US2010254020 A1 US 2010254020A1
Authority
US
United States
Prior art keywords
laser beam
collimated
lens
planar
line generator
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
US12/418,710
Other versions
US7821718B1 (en
Inventor
Alexander Govyadinov
Lenward Seals
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Hewlett Packard Development Co LP
Original Assignee
Hewlett Packard Development Co LP
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Hewlett Packard Development Co LP filed Critical Hewlett Packard Development Co LP
Priority to US12/418,710 priority Critical patent/US7821718B1/en
Assigned to HEWLETT-PACKARD DEVELOPMENT COMPANY, L.P. reassignment HEWLETT-PACKARD DEVELOPMENT COMPANY, L.P. ASSIGNMENT OF ASSIGNORS INTEREST (SEE DOCUMENT FOR DETAILS). Assignors: SEALS, LENWARD, GOVYADINOV, ALEXANDER
Publication of US20100254020A1 publication Critical patent/US20100254020A1/en
Application granted granted Critical
Publication of US7821718B1 publication Critical patent/US7821718B1/en
Active legal-status Critical Current
Adjusted expiration legal-status Critical

Links

Images

Classifications

    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/30Collimators
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B19/00Condensers, e.g. light collectors or similar non-imaging optics
    • G02B19/0004Condensers, e.g. light collectors or similar non-imaging optics characterised by the optical means employed
    • G02B19/0009Condensers, e.g. light collectors or similar non-imaging optics characterised by the optical means employed having refractive surfaces only
    • G02B19/0014Condensers, e.g. light collectors or similar non-imaging optics characterised by the optical means employed having refractive surfaces only at least one surface having optical power
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B19/00Condensers, e.g. light collectors or similar non-imaging optics
    • G02B19/0033Condensers, e.g. light collectors or similar non-imaging optics characterised by the use
    • G02B19/0047Condensers, e.g. light collectors or similar non-imaging optics characterised by the use for use with a light source
    • G02B19/0052Condensers, e.g. light collectors or similar non-imaging optics characterised by the use for use with a light source the light source comprising a laser diode
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/09Beam shaping, e.g. changing the cross-sectional area, not otherwise provided for
    • G02B27/0938Using specific optical elements
    • G02B27/0944Diffractive optical elements, e.g. gratings, holograms
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/09Beam shaping, e.g. changing the cross-sectional area, not otherwise provided for
    • G02B27/0938Using specific optical elements
    • G02B27/095Refractive optical elements
    • G02B27/0955Lenses
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S5/00Semiconductor lasers
    • H01S5/005Optical components external to the laser cavity, specially adapted therefor, e.g. for homogenisation or merging of the beams or for manipulating laser pulses, e.g. pulse shaping
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01SDEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL
    • H01S5/00Semiconductor lasers
    • H01S5/02Structural details or components not essential to laser action
    • H01S5/022Mountings; Housings
    • H01S5/0225Out-coupling of light
    • H01S5/02253Out-coupling of light using lenses

Definitions

  • Lasers are used in a multitude of devices and applications.
  • a typical laser emits a beam having a disc-like cross-section and Gaussian energy distribution.
  • Many such laser beams strikes a target as a “spot” of energy having peak intensity at its center, the intensity decreasing radially in a characteristic non-linear manner.
  • Some applications require laser beam energy having other than a disc-like or elliptical cross-sectional distribution. Additionally, it is desirable to provide such other laser beam patterns in an economical manner and with a minimum of apparatus complexity.
  • FIG. 1 depicts a schematic view of an optical system according to an embodiment
  • FIG. 2 depicts a schematic view of an optical system according to an embodiment
  • FIG. 3 depicts a schematic view of an optical system according to an embodiment
  • FIG. 4 depicts a schematic view of an optical system according to an embodiment
  • FIG. 5 depicts a schematic view of an optical system according to an embodiment
  • FIG. 5A depicts a schematic view of a compound optical element according to one embodiment
  • FIG. 6 depicts a schematic view of an optical system according to an embodiment
  • FIG. 7 depicts a schematic view of an optical system according to an embodiment
  • FIG. 7A depicts a schematic view of an integrated optical assembly according to an embodiment
  • FIG. 7B depicts a schematic view of an integrated optical assembly according to an embodiment
  • FIG. 7C depicts a schematic view of an integrated optical assembly according to an embodiment
  • FIG. 8 depicts an isometric block diagram of an operating scenario according to one embodiment
  • FIG. 9 depicts a schematic view of a packaged laser device according to one embodiment
  • FIG. 9A depicts an end detail view of the embodiment of FIG. 9 ;
  • FIG. 10 depicts a schematic view of a packaged laser device according to one embodiment
  • FIG. 10A depicts an end detail view of the embodiment of FIG. 10 .
  • a laser emitter generates a laser beam.
  • Optics disposed within the path of the laser beam function to shape and collimate the laser beam in at least one axis such that a generally flattened, planar laser beam is derived.
  • Such a planar laser beam has a substantially rectangular or line-like cross-sectional pattern.
  • the planar laser beams according to the present teachings can be used in ink drop detection and/or other applications.
  • an apparatus in one embodiment, includes a line generator that is configured to shape a collimated laser beam into an expanding planar laser beam.
  • the line generator includes at least one planar surface through which the expanding planar laser beam passes.
  • the apparatus also includes a collimator configured to collimate the expanding planar laser beam in at least a fast axis or a slow axis, such that a collimated planar laser beam is derived.
  • an optical apparatus in another embodiment, includes a solid-state laser configured to emit a laser beam.
  • the apparatus also includes first collimation optics configured to shape the laser beam into a collimated laser beam.
  • line generator optics configured to shape the collimated laser beam into an expanding planar laser beam.
  • the line generator optics include a planar optical surface through which the expanding planar laser beam passes.
  • the apparatus further includes second collimation optics configured to shape the expanding planar laser beam into a collimated planar laser beam.
  • an integrated apparatus in yet another embodiment, includes a packaging, and a laser emitter supported by the packaging.
  • the integrated apparatus also includes collimation optics supported by the packaging.
  • the collimation optics is configured to collimate a laser beam emitted by the laser emitter.
  • line generator optics is supported by the packaging and is configured to shape the collimated laser beam into a planer laser beam having about a rectangular cross-section.
  • the integrated apparatus further includes a slit supported by the packaging. The slit is configured to limit at least a width dimension or a thickness dimension of the planar laser beam as it propagates from the packaging.
  • FIG. 1 depicts a schematic view of an optical system 100 according to one embodiment.
  • the system 100 is illustrative and non-limiting with respect to the present teachings. Thus, other systems can also be defined, produced and used according to the present teachings.
  • the system 100 includes a laser emitter (i.e., laser) 102 .
  • the laser 102 can be, for non-limiting example, a solid-state laser diode, an edge emitter laser, a vertical-cavity surface-emitting laser (VCSEL), a gas-based laser, a ruby laser, etc. Other suitable lasers can also be used.
  • the laser 102 is configured to emit a laser beam 104 .
  • the system includes an aspheric lens 106 .
  • the lens 106 is disposed within the path of the laser beam 104 .
  • the lens 106 is configured to collimate (i.e., shape) the laser beam 104 such that a laser beam 108 that is collimated to some degree in at least one or both optical axis is produced. That is, the beam 108 is further collimated relative to laser beam 104 .
  • the lens 106 can also be considered a collimator 106 for purposes of the present teachings.
  • the system 100 also includes a diffraction grating 110 disposed within the path of the collimated laser beam 108 .
  • the diffraction grating 110 is configured to shape the collimated laser beam 108 into a generally planar beam 112 .
  • the beam 112 has an expanding width-wise dimension as it propagates away from the diffraction grating 110 , and has a substantially constant thickness-wise dimension.
  • the beam 112 is also referred to as an expanding planar laser beam 112 for purposes herein.
  • the diffraction grating 110 includes at least one planar side 110 A through which the expanding planar laser beam 112 passes.
  • the system 100 also includes a cylindrical lens 114 .
  • the lens 114 is disposed within the path of the expanding planar laser beam 112 and acts to shape a planar laser beam 116 that is collimated in both the fast axis and the slow axis. Additionally, a portion 118 of the expanding planar laser beam 112 passes through the lens 114 that is collimated in the fast (or slow) axis only.
  • the lens 114 can also be considered a collimator 114 for purposes of the present teachings.
  • the system 100 serves to shape (or derive) an original (or source) laser beam 104 having a typical disc-like (or elliptical), Gaussian distribution pattern into a collimated, planar laser beam 116 having a cross-section that is elongated in a width-wise dimension and flattened (i.e., narrowed) in a thickness-wise dimension.
  • a planar laser beam 116 strikes a flat target normal thereto as a line or generally rectangular region.
  • Table 1 below provides illustrative and non-limiting examples of commercially available elements that can be used to assemble the system 100 .
  • Other respective suitable elements i.e., parts or components
  • FIG. 2 depicts a schematic view of an optical system 200 according to one embodiment.
  • the system 200 is illustrative and non-limiting with respect to the present teachings. Thus, other systems can also be defined, produced and used according to the present teachings.
  • the system 200 includes a laser emitter (i.e., laser) 202 .
  • the laser 102 can be defined substantially as described above with respect to the laser 102 .
  • Other suitable lasers can also be used.
  • the laser 202 is configured to emit a laser beam 204 .
  • the system 200 also includes an aspheric lens 206 .
  • the lens 206 is disposed within the path of the laser beam 204 and is configured to shape the laser beam 204 such that a collimated laser beam 208 is produced. In this way, the lens 206 can be considered a collimator 206 for purposes of the present teachings.
  • the system 200 also includes a diffraction grating 210 disposed within the path of the collimated laser beam 208 .
  • the diffraction grating 210 is substantially as defined above with respect to the diffraction grating 110 , and is configured to shape the collimated laser beam 208 into an expanding, generally planar beam 212 .
  • the beam 212 is also referred to as an expanding planar laser beam 212 for purposes herein. It is noted that the diffraction grating 210 includes at least one planar side 210 A through which the expanding planar laser beam 212 passes.
  • the system 200 also includes a Fresnel cylindrical lens 214 .
  • the Fresnel lens 214 is disposed within the path of and acts to collimate the expanding planar laser beam 212 in one chosen axis. As depicted in FIG. 2 , it is the fast axis that is collimated. As such, a collimated planar laser beam 216 having a substantially linear or substantially rectangular cross-sectional energy distribution pattern is derived.
  • the Fresnel lens 214 can also be referred to as a collimator 214 for purposes of the present teachings.
  • the system 200 serves to shape a laser beam 204 having a typical Gaussian distribution pattern into a collimated, planar laser beam 216 having a cross-section having a generally constant width-wise dimension and a flattened, generally constant thickness-wise dimension.
  • a planar laser beam 216 strikes a flat target normal thereto as a line or generally rectangular region (see FIG. 8 ).
  • Table 2 below provides illustrative and non-limiting examples of commercially available elements that can be used to assemble the system 200 . Other respective suitable elements can also be used.
  • FIG. 3 depicts a schematic view of an optical system 300 according to one embodiment.
  • the system 300 is illustrative and non-limiting with respect to the present teachings. Thus, other systems can also be defined produced and used according to the present teachings.
  • the system 300 includes a laser emitter (i.e., laser) 302 .
  • the laser 302 can be defined substantially as described above with respect to the laser 102 . Other suitable lasers can also be used.
  • the laser 302 is configured to emit a laser beam 304 .
  • the system includes an aspheric lens 306 .
  • the lens 306 can be any suitable aspheric lens with focal length of 0.65 mm.
  • the lens 306 is disposed within the path of the laser beam 304 and is configured to shape the laser beam 304 such that collimated laser beam 308 is produced.
  • the lens 306 can be considered a collimator 306 for purposes of the present teachings.
  • the system 300 also includes an integrated optical element 310 .
  • the optical element 310 includes a diffraction grating 312 disposed within the path of the collimated laser beam 308 .
  • the diffraction grating 312 is configured to shape the collimated laser beam 308 into an expanding, generally planar laser beam 314 .
  • the beam 314 is also referred to as an expanding planar laser beam 314 for purposes herein. It is noted that the diffraction grating 312 includes at least one planar side 312 A through which the expanding planar laser beam 314 passes.
  • the integrated optical element 310 includes a mass of solid transparent material 316 .
  • the transparent material 316 can be defined by transparent media such as acrylic glass, BK7 glass etc. Other integrated optical elements or assemblages 310 having respectively varying materials 316 can also be used.
  • the diffraction grating 312 is set within, cemented to, or defined by the transparent material 316 .
  • the transparent material 316 molded, scribed or otherwise formed to define the diffraction grating 312 , such that the optical element 310 is defined by a monolithic structure. Other embodiments can also be used.
  • the integrated optical element 310 includes, or is configured to define, a cylindrical lens surface 318 .
  • the cylindrical lens surface 318 is configured to collimate the expanding planar laser beam 314 in one chosen axis, which is fast axis in the example.
  • the optical element 310 is custom formed, having a combination of a diffractive element (diffraction grating) 312 of twenty-five hundred lines per mm, and a cylindrical lens with a focal length of 6 mm.
  • a collimated planar laser beam 320 having a substantially linear or rectangular cross-section is derived and propagates away from the integrated optical element 310 .
  • the system 300 serves to shape a laser beam 304 having a typical Gaussian distribution pattern into a collimated, planar laser beam 320 having a cross-section that is elongated in a width-wise dimension and generally flattened in a thickness-wise dimension.
  • a planar laser beam 320 strikes a flat target normal thereto as a line or generally rectangular region (see FIG. 8 ).
  • Table 3 below provides illustrative and non-limiting examples of commercially available elements that can be used to assemble the system 300 . Other respective suitable elements can also be used.
  • FIG. 4 depicts a schematic view of an optical system 400 according to one embodiment.
  • the system 400 is illustrative and non-limiting with respect to the present teachings. Thus, other systems can also be defined, produced and used according to the present teachings.
  • the system 400 includes a laser emitter (i.e., laser) 402 .
  • the laser 402 can be defined substantially as described above with respect to the laser 102 . Other suitable lasers can also be used.
  • the laser 402 is configured to emit a laser beam 404 .
  • the system includes an aspheric lens 406 disposed within the path of the laser beam 404 and configured to shape the laser beam 404 such that collimated laser beam 408 is produced.
  • the lens 406 can be considered a collimator 406 for purposes of the present teachings.
  • the system 400 also includes an integrated optical element 410 .
  • the optical element 410 includes a diffraction grating 412 disposed within the path of the collimated laser beam 408 .
  • the diffraction grating 412 is configured to shape the collimated laser beam 408 into an expanding, generally planar laser beam 414 . It is noted that the diffraction grating 412 includes at least one planar side 412 A through which the expanding planar laser beam 414 passes.
  • the integrated optical element 410 includes a mass of solid transparent material 416 .
  • the transparent material 416 can be defined by transparent media such as acrylic glass, BK7 glass etc. Other integrated optical elements or assemblages 410 having respectively varying materials 416 can also be used.
  • the diffraction grating 412 is set within, cemented to, or defined by the transparent material 416 .
  • the integrated optical element 410 includes, or is configured to define, a Fresnel cylindrical lens surface 418 .
  • the Fresnel lens surface 418 is configured to collimate the expanding planar laser beam 414 in one axis as determined by the system design.
  • the Fresnel lens surface 418 can be defined by, or cemented to, the transparent material 416 .
  • a collimated planar laser beam 420 having a substantially linear or rectangular cross-sectional energy distribution pattern is derived and propagates away from the integrated optical element 410 .
  • the optical element 410 is custom formed, having a combination of diffractive element (diffraction grating) 412 of twenty-five hundred lines per mm, and a cylindrical lens with a focal length of 152.4 mm (6 inches), cemented together.
  • Other embodiments e.g., monolithic, etc. are possible.
  • the system 400 operates to provide a collimated, planar laser beam 420 having a cross-section that is elongated in a width-wise dimension and generally flattened in a thickness-wise dimension.
  • a planar laser beam 420 strikes a target normal thereto as a line or generally rectangular energy region.
  • Table 4 below provides illustrative and non-limiting examples of commercially available elements that can be used to assemble the system 400 . Other respective suitable elements can also be used.
  • FIG. 5 depicts a schematic view of an optical system 500 according to one embodiment.
  • the system 500 is illustrative and non-limiting with respect to the present teachings. Thus, other systems can also be defined, produced and used according to the present teachings.
  • the system 500 includes a laser emitter 502 and an aspheric lens 506 that are defined and configured substantially as described above with respect to the laser 402 and the lens 406 , respectively.
  • the laser 502 is configured to emit a laser beam 504 .
  • the aspheric lens 506 is disposed and configured to shape the laser beam 504 such that a collimated laser beam 508 is produced.
  • Lens 506 is an aspheric lens with focal length 0.65 mm.
  • the lens 506 can be considered a collimator 506 for purposes of the present teachings.
  • the system 500 also includes an integrated optical element 510 .
  • the optical element 510 includes a lenticular lens array 512 disposed within the path of the collimated laser beam 508 .
  • the lenticular lens array 512 is configured to shape the collimated laser beam 508 into an expanding, generally planar laser beam 514 (expanding planar laser beam 514 ). It is noted that the lenticular lens array 512 includes at least one planar side 512 A through which the expanding planar laser beam 514 passes.
  • the integrated optical element 510 includes a mass of solid transparent material 516 .
  • the transparent material 516 can be defined by transparent media such as acrylic glass, BK7 glass etc. Other integrated optical elements 510 having respectively varying materials 516 can also be used.
  • the lenticular lens array 512 is set within, cemented to, or defined by the transparent material 516 .
  • the integrated optical element 510 includes, or is configured to define, an acylindrical lens surface 518 .
  • the acylindrical lens surface 518 is configured to collimate the expanding planar laser beam 514 in both the fast axis and the slow axis.
  • a collimated planar laser beam 520 having a substantially linear or rectangular cross-sectional energy distribution pattern is derived and propagates away from the integrated optical element 510 .
  • the optical element 510 is a custom element, which is a combination of lenticular lens array 512 with a focal length of 2.16 mm (0.085 inches) and an acylindrical custom lens with a focal length of 6 mm, for example, cemented together.
  • Other embodiments, such as monolithic structures, can also be used.
  • the system 500 operates to provide a collimated, planar laser beam 520 having a cross-section that is elongated in a width-wise dimension and generally flattened in a thickness-wise dimension. It is noted that the lenticular lens array 512 operates to diverge/enlarge the laser beam 514 in one axis, while the aspheric surface 518 operates to provide a specific degree of collimation.
  • Table 5 below provides illustrative and non-limiting examples of commercially available elements that can be used to assemble the system 500 . Other respective suitable elements can also be used.
  • FIG. 5A depicts a compound optical element 550 .
  • the compound optical element 550 can be used in place of the integrated optical element 510 depicted in FIG. 5 .
  • the compound optical element 550 includes a mass of solid transparent material 552 .
  • the compound optical element 550 includes, or is configured to define, a lenticular lens array surface 554 .
  • the lenticular lens array surface 554 is configured to shape a collimated laser beam (e.g., 508 ) into an expanding planar laser beam (e.g., 514 ).
  • the compound optical element 550 includes, or is configured to define, an acylindrical lens surface 556 .
  • the acylindrical lens surface 556 is configured to collimate the expanding planar laser beam (e.g., 514 ) in both the fast axis and the slow axis.
  • a collimated planar laser beam (e.g., 520 ) having a substantially linear or rectangular cross-sectional energy distribution pattern is derived and propagates away from the integrated optical element 550 during normal operation.
  • the compound optical element 550 operates to provide a collimated, planar laser beam (e.g., 520 ) having a cross-section that is elongated in a width-wise dimension and generally flattened in a thickness-wise dimension.
  • a collimated, planar laser beam e.g., 520
  • Other suitable compound optical elements can also be used.
  • FIG. 6 depicts a schematic view of an optical system 600 according to one embodiment.
  • the system 600 is illustrative and non-limiting with respect to the present teachings. Thus, other systems can also be defined, produced and used according to the present teachings.
  • the system 600 includes a laser emitter 602 and an aspheric lens 606 that are defined and configured substantially as described above with respect to the laser 102 and the lens 106 , respectively.
  • the laser 602 is configured to emit a laser beam 604 .
  • the aspheric lens 606 is disposed and configured to shape the laser beam 604 such that a collimated laser beam 608 is produced.
  • the lens 606 is an aspheric lens with focal length of 0.65 mm.
  • the lens 606 can be considered a collimator 606 for purposes of the present teachings.
  • the system 600 also includes an integrated optical element 610 .
  • the optical element 610 includes a lenticular lens array surface 612 disposed within the path of the collimated laser beam 608 .
  • the lenticular lens array surface 612 is configured to shape the collimated laser beam 608 into an expanding planar laser beam 614 . It is noted that the lenticular lens array surface 612 includes at least one planar side 612 A through which the expanding planar laser beam 614 passes.
  • the integrated optical element 610 includes a mass of solid transparent material 616 .
  • the transparent material 616 can include a refractive transparent media such as acrylic glass, BK7 glass etc. Other integrated optical elements 610 having respectively varying materials 616 can also be used.
  • the lenticular lens array surface 612 is set within, cemented to, or defined by, the transparent material 616 .
  • the integrated optical element 610 includes, or is configured to define, a Fresnel cylindrical lens surface 618 .
  • the Fresnel cylindrical lens surface 618 is configured to collimate the expanding planar laser beam 614 in both the one axis.
  • a collimated planar laser beam 620 having a generally linear or rectangular cross-sectional energy distribution pattern is derived and propagates away from the integrated optical element 610 .
  • the optical element 610 is a custom element which is a combination of lenticular array 612 with a focal length of 2.16 mm (0.085 inches), and Fresnel acylindrical custom lens with a focal length of 6 mm, cemented together.
  • Other embodiments can also be used (e.g., monolithic structures, etc.).
  • the system 600 operates to provide a collimated, planar laser beam 620 having a cross-section that is elongated in a width-wise dimension and generally flattened in a thickness-wise dimension.
  • Table 6 below provides illustrative and non-limiting examples of commercially available elements that can be used to assemble the system 600 . Other respective suitable elements can also be used.
  • FIG. 7 depicts a schematic view of an optical system 700 according to one embodiment.
  • the system 700 is illustrative and non-limiting with respect to the present teachings. Thus, other systems can also be defined, produced and used according to the present teachings.
  • the system 700 includes a laser emitter (i.e., laser) 702 .
  • the laser 702 can be defined substantially as described above with respect to the laser 102 . Other suitable lasers can also be used.
  • the laser 702 is configured to emit a laser beam 704 .
  • the system includes an aspheric lens 706 disposed within the path of the laser beam 704 and configured to shape the laser beam 704 such that a collimated laser beam 708 is produced.
  • the lens 706 can be considered a collimator 706 for purposes of the present teachings.
  • the system 700 also includes an integrated optical assembly 710 .
  • the optical assembly 710 includes a beam shaping element 712 disposed within the path of the collimated laser beam 708 .
  • the beam shaping element 712 is configured to shape the collimated laser beam 708 into an expanding planar laser beam 714 . It is noted that the beam shaping element 712 includes at least one planar side 712 A through which the expanding planar laser beam 714 passes.
  • the beam shaping element 712 can be variously defined as described below in regard to FIGS. 7A , 7 B and 7 C, inclusive.
  • the integrated optical assembly 710 includes a mass of solid transparent material 716 .
  • the transparent material 716 is characterized by a refractive index that matches that of the beam shaping element 712 .
  • the transparent material 716 can be any transparent material compatible with the operating wavelength such as acrylic glass, BK7 glass etc.
  • the transparent material 716 can have a refractive index specifically defined for system application such as, for non-limiting example, 1.52, 1.4, or any material selected to match the optical characteristics of the system. Other suitable materials can also be used.
  • the beam shaping element 712 is bonded (cemented) to (or set within) and supported by the transparent material 716 .
  • the integrated optical assembly 710 includes a collimator 718 disposed within the path of the expanding planar laser beam 714 .
  • the collimator 718 is bonded to and supported by the transparent material 716 . Additionally, the collimator 718 is characterized by a refractive index that matches that of both the beam shaping element 712 and the transparent material 716 .
  • the collimator 718 can be variously defined as described below in regard to FIGS. 7A , 7 B and 7 C, inclusive.
  • the collimator 718 is configured to collimate the expanding planar laser beam 714 in one axis. As such, a collimated planar laser beam 720 having a generally linear or rectangular cross-sectional energy distribution pattern is derived and propagates away from the integrated optical assembly 710 .
  • FIG. 7A depicts an integrated optical assembly 730 that can be used in place of the integrated optical element 710 depicted in FIG. 7 .
  • the integrated optical assembly 730 includes a mass of solid transparent material 732 , a lenticular lens array surface 732 (i.e., beam shaping element), and a Fresnel cylindrical lens surface 736 (i.e., collimator).
  • the optical element 730 is a custom element which is a combination of a lenticular lens array 734 with a focal length of 2.16 mm (0.085 inches) and a Fresnel acylindrical custom lens 736 with a focal length of 6 mm, cemented together with custom glass block 732 of 10 mm thickness.
  • the optical assembly 730 is defined by a monolithic structure.
  • Table 7 below provides illustrative and non-limiting examples of commercially available elements that can be used to assemble the integrated optical assembly 730 . Other respective suitable elements can also be used.
  • FIG. 7 b depicts an integrated optical assembly 740 that can be used in place of the integrated optical element 710 depicted in FIG. 7 .
  • the integrated optical assembly 740 includes a mass of solid transparent material 742 , a diffraction grating surface 744 (i.e., beam shaping element), and a Fresnel cylindrical lens surface 746 (i.e., collimator).
  • the optical element 740 is a custom element which is a combination of diffractive element 744 of twenty-five hundred lines/mm, and Fresnel lens 746 with a focal length of 6 mm, cemented together by custom glass 742 of 10 mm thickness.
  • the optical assembly 740 is defined by a monolithic structure.
  • Table 8 below provides illustrative and non-limiting examples of commercially available elements that can be used to assemble the integrated optical assembly 740 . Other respective suitable elements can also be used.
  • FIG. 7C depicts an integrated optical assembly 750 that can be used in place of the integrated optical element 710 depicted in FIG. 7 .
  • the integrated optical assembly 750 includes a mass of solid transparent material 752 , a lenticular lens array surface 754 (i.e., beam shaping element), and an acylindrical or cylindrical lens surface 756 (i.e., collimator), depending on desired performance level.
  • the optical assembly 750 is defined by a monolithic structure.
  • FIG. 8 depicts an isometric block diagram of an operating scenario (i.e., operation) 800 according to the present teachings.
  • the operation 800 is illustrative and non-limiting in nature, and is directed to a clear understanding the present teachings. Other operations consistent with the present teachings can also be used.
  • the operation 800 includes a device (system or assembly) 802 configured to provide a collimated, planar beam of laser energy 804 .
  • the device 802 can be defined by any suitable such device or apparatus according to the present teachings such as, for non-limiting example, system 200 , 300 , 400 , etc., as described above or the device 900 or 1000 , etc., as described below. Other devices or systems in accordance with the present teachings can also be used.
  • a flat target 806 is disposed normal to the path of the laser beam 804 .
  • the laser beam 804 strikes the target 806 as a line of energy 808 .
  • an original (i.e., source) beam of laser energy (not shown) generated within the device 802 has been shaped so as to strike the target 806 as a line-like or narrow, substantially rectangular area 808 .
  • FIG. 9 depicts a packaged laser device 900 according to another embodiment.
  • the device 900 is illustrative and non-limiting with respect to the present teachings.
  • Other packaged devices can also be configured and/or used according to the present teachings.
  • the device 900 includes a holder tube (i.e., packaging or housing) 902 .
  • the holder tube 902 can be formed from any suitable material such as, for non-limiting example, aluminum, stainless steel, etc. Other materials can also be used.
  • the holder tube 902 is configured to protectively house a plurality of elements described hereinafter.
  • the device 900 also includes an edge emitter laser 904 .
  • the laser 904 is configured to provide a beam of laser energy.
  • the laser 904 is analogous in operation to the lasers 102 , 202 , etc. as described above.
  • the laser 904 is supported at one end of the holder tube 902 .
  • the device 900 also includes collimation optics 906 .
  • the collimation optics 906 are configured to collimate a beam emitted by the laser 904 .
  • the collimation optics 906 are defined by an aspheric lens. Other suitable collimation optics can also be used.
  • the collimation optics 906 are analogous to the collimators 106 , 206 , etc. as described above.
  • the collimation optics 906 are supported within the holder tube 902 .
  • the device 900 includes line generator 908 .
  • the line generator 908 is configured to shape the collimated laser beam propagating from the collimation optics 906 into a generally flattened, collimated planar laser beam.
  • the line generator 908 is defined by an integrated optical element such as, for non-limiting example, the integrated optical elements 310 , 410 , 510 , etc. Other suitable line generators 908 can also be used.
  • the device 900 also includes a slit 910 defined in an end plug 912 .
  • FIG. 9A depicts an end elevation view of details of the device 900 .
  • the slit 910 is configured to limit width-wise and thickness-wise dimensions of the laser beam emitted from the device 900 during normal operation. In this way, a laser beam having a flattened, generally rectangular cross-sectional energy distribution pattern is provided by the device 900 during normal use.
  • Support elements 914 and 916 are further included within the device 900 so as to fixedly support and space collimation optics 906 and line generator 908 . Additionally, an optional spatial filter (not shown) can be included within or adjacent to the slit 910 .
  • the device 900 provides an integrated assemblage of elements configured to generate a laser beam having a line-like or rectangular cross-sectional energy distribution of generally constant width and thickness dimensions.
  • the device 900 is applicable, for non-limiting example, in an inkjet printing context to perform drop detection testing of the ink emitter dies. Other suitable applications are also possible.
  • FIG. 10 depicts a packaged laser device 1000 according to another embodiment.
  • the device 1000 is illustrative and non-limiting with respect to the present teachings.
  • Other packaged devices can also be configured and/or used according to the present teachings.
  • the device 1000 includes a holder tube (i.e., packaging or housing) 1002 .
  • the holder tube 1002 can be formed from any suitable material such as, for non-limiting example, aluminum, stainless steel, etc. Other materials can also be used.
  • the holder tube 1002 is configured to protectively house a plurality of elements described hereinafter.
  • the device 1000 also includes a vertical-cavity surface-emitting laser (VCSEL) 1004 .
  • the laser 1004 is configured to provide a beam of laser energy.
  • the laser 1004 is analogous in operation to the lasers 102 , 202 , etc. as described above.
  • the laser 1004 is supported at one end of the holder tube 1002 .
  • the device 1000 also includes optional collimation optics 1006 .
  • the collimation optics 1006 are configured to collimate a beam emitted by the laser 1004 .
  • the collimation optics 1006 include a spheric or aspheric lens. Other suitable collimation optics can also be used.
  • the collimation optics 1006 are analogous to the collimators 106 , 206 , etc. as described above.
  • the collimation optics 1006 is supported within the holder tube 1002 or in VCSEL package.
  • the device 1000 includes a line generator 1008 .
  • the line generator 1008 is configured to shape the collimated laser beam propagating from the (optional) collimation optics 1006 into a generally flattened, collimated planar laser beam.
  • the line generator 1008 is defined by an integrated optical element such as, for non-limiting example, the integrated optical elements 310 , 410 , 510 , etc. Other suitable line generators 1008 can also be used.
  • the device 1000 also includes a slit 1010 defined in an end plug 1012 .
  • FIG. 10A depicts an end elevation view of details of the device 1000 .
  • the slit 1010 is configured to limit a width-wise dimension and a thickness-wise dimension of the laser beam emitted from the device 1000 during normal operation. In this way, a laser beam having a flattened, rectangular cross-sectional pattern is provided by the device 1000 during normal use.
  • Support elements 1014 and 1016 are further included within the device 1000 so as to fixedly support and space collimation optics 1006 and line generator 1008 . Additionally, a spatial filter (not shown) can be optionally included within or adjacent to the slit 1010 .
  • the device 1000 provides an integrated assemblage of elements configured to generate a laser beam having a line-like or rectangular cross-sectional energy distribution of generally constant width and thickness dimensions.
  • the device 1000 is applicable, for non-limiting example, in an inkjet printing context to perform drop detection testing of the ink emission nozzles. Other suitable applications are also possible.

Abstract

A laser beam emission is collimated by optics. The collimated beam is shaped into an expanding planar laser beam by line generator optics. The expanding planar laser beam is collimated by other optics such that a beam having a generally rectangular cross-section is derived. The resulting beam can be used in ink drop detection and/or other applications.

Description

    BACKGROUND
  • Lasers are used in a multitude of devices and applications. A typical laser emits a beam having a disc-like cross-section and Gaussian energy distribution. Many such laser beams strikes a target as a “spot” of energy having peak intensity at its center, the intensity decreasing radially in a characteristic non-linear manner.
  • Some applications require laser beam energy having other than a disc-like or elliptical cross-sectional distribution. Additionally, it is desirable to provide such other laser beam patterns in an economical manner and with a minimum of apparatus complexity.
  • Accordingly, the embodiments described hereinafter were developed in the interest of addressing the foregoing needs and problems.
  • BRIEF DESCRIPTION OF THE DRAWINGS
  • The present embodiments will now be described, by way of example, with reference to the accompanying drawings, in which:
  • FIG. 1 depicts a schematic view of an optical system according to an embodiment;
  • FIG. 2 depicts a schematic view of an optical system according to an embodiment;
  • FIG. 3 depicts a schematic view of an optical system according to an embodiment;
  • FIG. 4 depicts a schematic view of an optical system according to an embodiment;
  • FIG. 5 depicts a schematic view of an optical system according to an embodiment;
  • FIG. 5A depicts a schematic view of a compound optical element according to one embodiment;
  • FIG. 6 depicts a schematic view of an optical system according to an embodiment;
  • FIG. 7 depicts a schematic view of an optical system according to an embodiment;
  • FIG. 7A depicts a schematic view of an integrated optical assembly according to an embodiment;
  • FIG. 7B depicts a schematic view of an integrated optical assembly according to an embodiment;
  • FIG. 7C depicts a schematic view of an integrated optical assembly according to an embodiment;
  • FIG. 8 depicts an isometric block diagram of an operating scenario according to one embodiment;
  • FIG. 9 depicts a schematic view of a packaged laser device according to one embodiment;
  • FIG. 9A depicts an end detail view of the embodiment of FIG. 9;
  • FIG. 10 depicts a schematic view of a packaged laser device according to one embodiment;
  • FIG. 10A depicts an end detail view of the embodiment of FIG. 10.
  • DETAILED DESCRIPTION Introduction
  • Means and methods for producing a planar laser beam are provided by the present teachings. A laser emitter generates a laser beam. Optics disposed within the path of the laser beam function to shape and collimate the laser beam in at least one axis such that a generally flattened, planar laser beam is derived. Such a planar laser beam has a substantially rectangular or line-like cross-sectional pattern. The planar laser beams according to the present teachings can be used in ink drop detection and/or other applications.
  • In one embodiment, an apparatus includes a line generator that is configured to shape a collimated laser beam into an expanding planar laser beam. The line generator includes at least one planar surface through which the expanding planar laser beam passes. The apparatus also includes a collimator configured to collimate the expanding planar laser beam in at least a fast axis or a slow axis, such that a collimated planar laser beam is derived.
  • In another embodiment, an optical apparatus includes a solid-state laser configured to emit a laser beam. The apparatus also includes first collimation optics configured to shape the laser beam into a collimated laser beam. Also included are line generator optics configured to shape the collimated laser beam into an expanding planar laser beam. The line generator optics include a planar optical surface through which the expanding planar laser beam passes. The apparatus further includes second collimation optics configured to shape the expanding planar laser beam into a collimated planar laser beam.
  • In yet another embodiment, an integrated apparatus includes a packaging, and a laser emitter supported by the packaging. The integrated apparatus also includes collimation optics supported by the packaging. The collimation optics is configured to collimate a laser beam emitted by the laser emitter. Additionally, line generator optics is supported by the packaging and is configured to shape the collimated laser beam into a planer laser beam having about a rectangular cross-section. The integrated apparatus further includes a slit supported by the packaging. The slit is configured to limit at least a width dimension or a thickness dimension of the planar laser beam as it propagates from the packaging.
  • First Illustrative Embodiment
  • FIG. 1 depicts a schematic view of an optical system 100 according to one embodiment. The system 100 is illustrative and non-limiting with respect to the present teachings. Thus, other systems can also be defined, produced and used according to the present teachings.
  • The system 100 includes a laser emitter (i.e., laser) 102. The laser 102 can be, for non-limiting example, a solid-state laser diode, an edge emitter laser, a vertical-cavity surface-emitting laser (VCSEL), a gas-based laser, a ruby laser, etc. Other suitable lasers can also be used. The laser 102 is configured to emit a laser beam 104.
  • The system includes an aspheric lens 106. The lens 106 is disposed within the path of the laser beam 104. The lens 106 is configured to collimate (i.e., shape) the laser beam 104 such that a laser beam 108 that is collimated to some degree in at least one or both optical axis is produced. That is, the beam 108 is further collimated relative to laser beam 104. In this way, the lens 106 can also be considered a collimator 106 for purposes of the present teachings.
  • The system 100 also includes a diffraction grating 110 disposed within the path of the collimated laser beam 108. The diffraction grating 110 is configured to shape the collimated laser beam 108 into a generally planar beam 112. The beam 112 has an expanding width-wise dimension as it propagates away from the diffraction grating 110, and has a substantially constant thickness-wise dimension. The beam 112 is also referred to as an expanding planar laser beam 112 for purposes herein. It is noted that the diffraction grating 110 includes at least one planar side 110A through which the expanding planar laser beam 112 passes.
  • The system 100 also includes a cylindrical lens 114. The lens 114 is disposed within the path of the expanding planar laser beam 112 and acts to shape a planar laser beam 116 that is collimated in both the fast axis and the slow axis. Additionally, a portion 118 of the expanding planar laser beam 112 passes through the lens 114 that is collimated in the fast (or slow) axis only. Thus, the lens 114 can also be considered a collimator 114 for purposes of the present teachings.
  • The system 100 serves to shape (or derive) an original (or source) laser beam 104 having a typical disc-like (or elliptical), Gaussian distribution pattern into a collimated, planar laser beam 116 having a cross-section that is elongated in a width-wise dimension and flattened (i.e., narrowed) in a thickness-wise dimension. Such a planar laser beam 116 strikes a flat target normal thereto as a line or generally rectangular region.
  • Table 1 below provides illustrative and non-limiting examples of commercially available elements that can be used to assemble the system 100. Other respective suitable elements (i.e., parts or components) can also be used.
  • TABLE 1
    Illustrative System 100 Elements
    Element Model/Designation Source/Manufacturer
    Laser
    102 OED-LDP65001E Lumex Inc
    Lens
    106 AL5040-B ThorLabs
    Grating
    110 NT48-585 Edmund Optics
    Lens
    114 NT46-107 Edmund Optics
  • Second Illustrative Embodiment
  • FIG. 2 depicts a schematic view of an optical system 200 according to one embodiment. The system 200 is illustrative and non-limiting with respect to the present teachings. Thus, other systems can also be defined, produced and used according to the present teachings.
  • The system 200 includes a laser emitter (i.e., laser) 202. The laser 102 can be defined substantially as described above with respect to the laser 102. Other suitable lasers can also be used. The laser 202 is configured to emit a laser beam 204. The system 200 also includes an aspheric lens 206. The lens 206 is disposed within the path of the laser beam 204 and is configured to shape the laser beam 204 such that a collimated laser beam 208 is produced. In this way, the lens 206 can be considered a collimator 206 for purposes of the present teachings.
  • The system 200 also includes a diffraction grating 210 disposed within the path of the collimated laser beam 208. The diffraction grating 210 is substantially as defined above with respect to the diffraction grating 110, and is configured to shape the collimated laser beam 208 into an expanding, generally planar beam 212. The beam 212 is also referred to as an expanding planar laser beam 212 for purposes herein. It is noted that the diffraction grating 210 includes at least one planar side 210A through which the expanding planar laser beam 212 passes.
  • The system 200 also includes a Fresnel cylindrical lens 214. The Fresnel lens 214 is disposed within the path of and acts to collimate the expanding planar laser beam 212 in one chosen axis. As depicted in FIG. 2, it is the fast axis that is collimated. As such, a collimated planar laser beam 216 having a substantially linear or substantially rectangular cross-sectional energy distribution pattern is derived. The Fresnel lens 214 can also be referred to as a collimator 214 for purposes of the present teachings.
  • The system 200 serves to shape a laser beam 204 having a typical Gaussian distribution pattern into a collimated, planar laser beam 216 having a cross-section having a generally constant width-wise dimension and a flattened, generally constant thickness-wise dimension. Such a planar laser beam 216 strikes a flat target normal thereto as a line or generally rectangular region (see FIG. 8).
  • Table 2 below provides illustrative and non-limiting examples of commercially available elements that can be used to assemble the system 200. Other respective suitable elements can also be used.
  • TABLE 2
    Illustrative System 200 Elements
    Element Model/Designation Source/Manufacturer
    Laser
    202 OED-LDP65001E Lumex Inc
    Lens
    206 AL5040-B ThorLabs
    Grating
    210 NT48-585 Edmund Optics
    Cyl. F. Lens 214 NT46-107 Edmund Optics
  • Third Illustrative Embodiment
  • FIG. 3 depicts a schematic view of an optical system 300 according to one embodiment. The system 300 is illustrative and non-limiting with respect to the present teachings. Thus, other systems can also be defined produced and used according to the present teachings.
  • The system 300 includes a laser emitter (i.e., laser) 302. The laser 302 can be defined substantially as described above with respect to the laser 102. Other suitable lasers can also be used. The laser 302 is configured to emit a laser beam 304. The system includes an aspheric lens 306. The lens 306 can be any suitable aspheric lens with focal length of 0.65 mm. The lens 306 is disposed within the path of the laser beam 304 and is configured to shape the laser beam 304 such that collimated laser beam 308 is produced. The lens 306 can be considered a collimator 306 for purposes of the present teachings.
  • The system 300 also includes an integrated optical element 310. The optical element 310 includes a diffraction grating 312 disposed within the path of the collimated laser beam 308. The diffraction grating 312 is configured to shape the collimated laser beam 308 into an expanding, generally planar laser beam 314. The beam 314 is also referred to as an expanding planar laser beam 314 for purposes herein. It is noted that the diffraction grating 312 includes at least one planar side 312A through which the expanding planar laser beam 314 passes.
  • The integrated optical element 310 includes a mass of solid transparent material 316. The transparent material 316 can be defined by transparent media such as acrylic glass, BK7 glass etc. Other integrated optical elements or assemblages 310 having respectively varying materials 316 can also be used. The diffraction grating 312 is set within, cemented to, or defined by the transparent material 316. Thus, in one embodiment, the transparent material 316 molded, scribed or otherwise formed to define the diffraction grating 312, such that the optical element 310 is defined by a monolithic structure. Other embodiments can also be used.
  • The integrated optical element 310 includes, or is configured to define, a cylindrical lens surface 318. The cylindrical lens surface 318 is configured to collimate the expanding planar laser beam 314 in one chosen axis, which is fast axis in the example. In one embodiment, the optical element 310 is custom formed, having a combination of a diffractive element (diffraction grating) 312 of twenty-five hundred lines per mm, and a cylindrical lens with a focal length of 6 mm.
  • As such, a collimated planar laser beam 320 having a substantially linear or rectangular cross-section is derived and propagates away from the integrated optical element 310.
  • The system 300 serves to shape a laser beam 304 having a typical Gaussian distribution pattern into a collimated, planar laser beam 320 having a cross-section that is elongated in a width-wise dimension and generally flattened in a thickness-wise dimension. Such a planar laser beam 320 strikes a flat target normal thereto as a line or generally rectangular region (see FIG. 8).
  • Table 3 below provides illustrative and non-limiting examples of commercially available elements that can be used to assemble the system 300. Other respective suitable elements can also be used.
  • TABLE 3
    Illustrative System 300 Elements
    Element Model/Designation Source/Manufacturer
    Laser
    302 OPV332 Optek Inc.
    Lens 306 aspheric F.L. = 0.65 mm
    Optical E. 310 custom custom made
  • Fourth Illustrative Embodiment
  • FIG. 4 depicts a schematic view of an optical system 400 according to one embodiment. The system 400 is illustrative and non-limiting with respect to the present teachings. Thus, other systems can also be defined, produced and used according to the present teachings.
  • The system 400 includes a laser emitter (i.e., laser) 402. The laser 402 can be defined substantially as described above with respect to the laser 102. Other suitable lasers can also be used. The laser 402 is configured to emit a laser beam 404. The system includes an aspheric lens 406 disposed within the path of the laser beam 404 and configured to shape the laser beam 404 such that collimated laser beam 408 is produced. The lens 406 can be considered a collimator 406 for purposes of the present teachings.
  • The system 400 also includes an integrated optical element 410. The optical element 410 includes a diffraction grating 412 disposed within the path of the collimated laser beam 408. The diffraction grating 412 is configured to shape the collimated laser beam 408 into an expanding, generally planar laser beam 414. It is noted that the diffraction grating 412 includes at least one planar side 412A through which the expanding planar laser beam 414 passes.
  • The integrated optical element 410 includes a mass of solid transparent material 416. The transparent material 416 can be defined by transparent media such as acrylic glass, BK7 glass etc. Other integrated optical elements or assemblages 410 having respectively varying materials 416 can also be used. The diffraction grating 412 is set within, cemented to, or defined by the transparent material 416. The integrated optical element 410 includes, or is configured to define, a Fresnel cylindrical lens surface 418. The Fresnel lens surface 418 is configured to collimate the expanding planar laser beam 414 in one axis as determined by the system design. The Fresnel lens surface 418 can be defined by, or cemented to, the transparent material 416.
  • As such, a collimated planar laser beam 420 having a substantially linear or rectangular cross-sectional energy distribution pattern is derived and propagates away from the integrated optical element 410. In one embodiment, the optical element 410 is custom formed, having a combination of diffractive element (diffraction grating) 412 of twenty-five hundred lines per mm, and a cylindrical lens with a focal length of 152.4 mm (6 inches), cemented together. Other embodiments (e.g., monolithic, etc.) are possible.
  • The system 400 operates to provide a collimated, planar laser beam 420 having a cross-section that is elongated in a width-wise dimension and generally flattened in a thickness-wise dimension. Such a planar laser beam 420 strikes a target normal thereto as a line or generally rectangular energy region.
  • Table 4 below provides illustrative and non-limiting examples of commercially available elements that can be used to assemble the system 400. Other respective suitable elements can also be used.
  • TABLE 4
    Illustrative System 400 Elements
    Element Model/Designation Source/Manufacturer
    Laser
    402 OPV332 Optek Inc.
    Lens 406 aspheric F.L. = 0.65 mm
    Optical E. 410 custom custom made
  • Fifth Illustrative Embodiment
  • FIG. 5 depicts a schematic view of an optical system 500 according to one embodiment. The system 500 is illustrative and non-limiting with respect to the present teachings. Thus, other systems can also be defined, produced and used according to the present teachings.
  • The system 500 includes a laser emitter 502 and an aspheric lens 506 that are defined and configured substantially as described above with respect to the laser 402 and the lens 406, respectively. The laser 502 is configured to emit a laser beam 504. In turn, the aspheric lens 506 is disposed and configured to shape the laser beam 504 such that a collimated laser beam 508 is produced. Lens 506 is an aspheric lens with focal length 0.65 mm. The lens 506 can be considered a collimator 506 for purposes of the present teachings.
  • The system 500 also includes an integrated optical element 510. The optical element 510 includes a lenticular lens array 512 disposed within the path of the collimated laser beam 508. The lenticular lens array 512 is configured to shape the collimated laser beam 508 into an expanding, generally planar laser beam 514 (expanding planar laser beam 514). It is noted that the lenticular lens array 512 includes at least one planar side 512A through which the expanding planar laser beam 514 passes.
  • The integrated optical element 510 includes a mass of solid transparent material 516. The transparent material 516 can be defined by transparent media such as acrylic glass, BK7 glass etc. Other integrated optical elements 510 having respectively varying materials 516 can also be used. The lenticular lens array 512 is set within, cemented to, or defined by the transparent material 516.
  • The integrated optical element 510 includes, or is configured to define, an acylindrical lens surface 518. The acylindrical lens surface 518 is configured to collimate the expanding planar laser beam 514 in both the fast axis and the slow axis. As such, a collimated planar laser beam 520 having a substantially linear or rectangular cross-sectional energy distribution pattern is derived and propagates away from the integrated optical element 510. In one embodiment, the optical element 510 is a custom element, which is a combination of lenticular lens array 512 with a focal length of 2.16 mm (0.085 inches) and an acylindrical custom lens with a focal length of 6 mm, for example, cemented together. Other embodiments, such as monolithic structures, can also be used.
  • The system 500 operates to provide a collimated, planar laser beam 520 having a cross-section that is elongated in a width-wise dimension and generally flattened in a thickness-wise dimension. It is noted that the lenticular lens array 512 operates to diverge/enlarge the laser beam 514 in one axis, while the aspheric surface 518 operates to provide a specific degree of collimation. Table 5 below provides illustrative and non-limiting examples of commercially available elements that can be used to assemble the system 500. Other respective suitable elements can also be used.
  • TABLE 5
    Illustrative System 500 Elements
    Element Model/Designation Source/Manufacturer
    Laser
    502 Opv332 Optek Inc.
    Lens 506 NT43-028 Edmund Optics
    Optical E. 510 Custom Custom made
  • FIG. 5A depicts a compound optical element 550. The compound optical element 550 can be used in place of the integrated optical element 510 depicted in FIG. 5. The compound optical element 550 includes a mass of solid transparent material 552. The compound optical element 550 includes, or is configured to define, a lenticular lens array surface 554. The lenticular lens array surface 554 is configured to shape a collimated laser beam (e.g., 508) into an expanding planar laser beam (e.g., 514).
  • The compound optical element 550 includes, or is configured to define, an acylindrical lens surface 556. The acylindrical lens surface 556 is configured to collimate the expanding planar laser beam (e.g., 514) in both the fast axis and the slow axis. As such, a collimated planar laser beam (e.g., 520) having a substantially linear or rectangular cross-sectional energy distribution pattern is derived and propagates away from the integrated optical element 550 during normal operation.
  • The compound optical element 550 operates to provide a collimated, planar laser beam (e.g., 520) having a cross-section that is elongated in a width-wise dimension and generally flattened in a thickness-wise dimension. Other suitable compound optical elements can also be used.
  • Sixth Illustrative Embodiment
  • FIG. 6 depicts a schematic view of an optical system 600 according to one embodiment. The system 600 is illustrative and non-limiting with respect to the present teachings. Thus, other systems can also be defined, produced and used according to the present teachings.
  • The system 600 includes a laser emitter 602 and an aspheric lens 606 that are defined and configured substantially as described above with respect to the laser 102 and the lens 106, respectively. The laser 602 is configured to emit a laser beam 604. In turn, the aspheric lens 606 is disposed and configured to shape the laser beam 604 such that a collimated laser beam 608 is produced. The lens 606 is an aspheric lens with focal length of 0.65 mm. The lens 606 can be considered a collimator 606 for purposes of the present teachings.
  • The system 600 also includes an integrated optical element 610. The optical element 610 includes a lenticular lens array surface 612 disposed within the path of the collimated laser beam 608. The lenticular lens array surface 612 is configured to shape the collimated laser beam 608 into an expanding planar laser beam 614. It is noted that the lenticular lens array surface 612 includes at least one planar side 612A through which the expanding planar laser beam 614 passes.
  • The integrated optical element 610 includes a mass of solid transparent material 616. The transparent material 616 can include a refractive transparent media such as acrylic glass, BK7 glass etc. Other integrated optical elements 610 having respectively varying materials 616 can also be used. The lenticular lens array surface 612 is set within, cemented to, or defined by, the transparent material 616.
  • The integrated optical element 610 includes, or is configured to define, a Fresnel cylindrical lens surface 618. The Fresnel cylindrical lens surface 618 is configured to collimate the expanding planar laser beam 614 in both the one axis. As such, a collimated planar laser beam 620 having a generally linear or rectangular cross-sectional energy distribution pattern is derived and propagates away from the integrated optical element 610. In one embodiment, the optical element 610 is a custom element which is a combination of lenticular array 612 with a focal length of 2.16 mm (0.085 inches), and Fresnel acylindrical custom lens with a focal length of 6 mm, cemented together. Other embodiments can also be used (e.g., monolithic structures, etc.).
  • The system 600 operates to provide a collimated, planar laser beam 620 having a cross-section that is elongated in a width-wise dimension and generally flattened in a thickness-wise dimension.
  • Table 6 below provides illustrative and non-limiting examples of commercially available elements that can be used to assemble the system 600. Other respective suitable elements can also be used.
  • TABLE 6
    Illustrative System 600 Elements
    Element Model/Designation Source/Manufacturer
    Laser
    602 Opv332 Optek Inc.
    Lens 606 NT43-028 Edmund Optics
    Optical E. 610 Custom Custom made
  • Seventh Illustrative Embodiment
  • FIG. 7 depicts a schematic view of an optical system 700 according to one embodiment. The system 700 is illustrative and non-limiting with respect to the present teachings. Thus, other systems can also be defined, produced and used according to the present teachings.
  • The system 700 includes a laser emitter (i.e., laser) 702. The laser 702 can be defined substantially as described above with respect to the laser 102. Other suitable lasers can also be used. The laser 702 is configured to emit a laser beam 704. The system includes an aspheric lens 706 disposed within the path of the laser beam 704 and configured to shape the laser beam 704 such that a collimated laser beam 708 is produced. The lens 706 can be considered a collimator 706 for purposes of the present teachings.
  • The system 700 also includes an integrated optical assembly 710. The optical assembly 710 includes a beam shaping element 712 disposed within the path of the collimated laser beam 708. The beam shaping element 712 is configured to shape the collimated laser beam 708 into an expanding planar laser beam 714. It is noted that the beam shaping element 712 includes at least one planar side 712A through which the expanding planar laser beam 714 passes. The beam shaping element 712 can be variously defined as described below in regard to FIGS. 7A, 7B and 7C, inclusive.
  • The integrated optical assembly 710 includes a mass of solid transparent material 716. The transparent material 716 is characterized by a refractive index that matches that of the beam shaping element 712. For non-limiting example, the transparent material 716 can be any transparent material compatible with the operating wavelength such as acrylic glass, BK7 glass etc. The transparent material 716 can have a refractive index specifically defined for system application such as, for non-limiting example, 1.52, 1.4, or any material selected to match the optical characteristics of the system. Other suitable materials can also be used. The beam shaping element 712 is bonded (cemented) to (or set within) and supported by the transparent material 716.
  • The integrated optical assembly 710 includes a collimator 718 disposed within the path of the expanding planar laser beam 714. The collimator 718 is bonded to and supported by the transparent material 716. Additionally, the collimator 718 is characterized by a refractive index that matches that of both the beam shaping element 712 and the transparent material 716. The collimator 718 can be variously defined as described below in regard to FIGS. 7A, 7B and 7C, inclusive. The collimator 718 is configured to collimate the expanding planar laser beam 714 in one axis. As such, a collimated planar laser beam 720 having a generally linear or rectangular cross-sectional energy distribution pattern is derived and propagates away from the integrated optical assembly 710.
  • FIG. 7A depicts an integrated optical assembly 730 that can be used in place of the integrated optical element 710 depicted in FIG. 7. The integrated optical assembly 730 includes a mass of solid transparent material 732, a lenticular lens array surface 732 (i.e., beam shaping element), and a Fresnel cylindrical lens surface 736 (i.e., collimator). In one embodiment, the optical element 730 is a custom element which is a combination of a lenticular lens array 734 with a focal length of 2.16 mm (0.085 inches) and a Fresnel acylindrical custom lens 736 with a focal length of 6 mm, cemented together with custom glass block 732 of 10 mm thickness. In another embodiment, the optical assembly 730 is defined by a monolithic structure.
  • Table 7 below provides illustrative and non-limiting examples of commercially available elements that can be used to assemble the integrated optical assembly 730. Other respective suitable elements can also be used.
  • TABLE 7
    Illustrative Assembly 730 Elements
    Element Model/Designation Source/Manufacturer
    Optical Mat. 732 custom BK7, 10 mm thick (any)
    Lens Surface 734 NT43-028 Edmund Optics
    Fresnel Lens
    736 NT46-114 Edmund Optics
  • FIG. 7 b depicts an integrated optical assembly 740 that can be used in place of the integrated optical element 710 depicted in FIG. 7. The integrated optical assembly 740 includes a mass of solid transparent material 742, a diffraction grating surface 744 (i.e., beam shaping element), and a Fresnel cylindrical lens surface 746 (i.e., collimator). In one embodiment, the optical element 740 is a custom element which is a combination of diffractive element 744 of twenty-five hundred lines/mm, and Fresnel lens 746 with a focal length of 6 mm, cemented together by custom glass 742 of 10 mm thickness. In another embodiment, the optical assembly 740 is defined by a monolithic structure.
  • Table 8 below provides illustrative and non-limiting examples of commercially available elements that can be used to assemble the integrated optical assembly 740. Other respective suitable elements can also be used.
  • TABLE 8
    Illustrative Assembly 740 Elements
    Element Model/Designation Source/Manufacturer
    Optical Mat. 742 BK7 glass, 10 mm thick (any)
    Grating 744 2500 lines/mm (any)
    Fresnel Lens 746 6 mm focal length (any)
  • FIG. 7C depicts an integrated optical assembly 750 that can be used in place of the integrated optical element 710 depicted in FIG. 7. The integrated optical assembly 750 includes a mass of solid transparent material 752, a lenticular lens array surface 754 (i.e., beam shaping element), and an acylindrical or cylindrical lens surface 756 (i.e., collimator), depending on desired performance level. In another embodiment, the optical assembly 750 is defined by a monolithic structure.
  • First Illustrative Operation
  • FIG. 8 depicts an isometric block diagram of an operating scenario (i.e., operation) 800 according to the present teachings. The operation 800 is illustrative and non-limiting in nature, and is directed to a clear understanding the present teachings. Other operations consistent with the present teachings can also be used.
  • The operation 800 includes a device (system or assembly) 802 configured to provide a collimated, planar beam of laser energy 804. The device 802 can be defined by any suitable such device or apparatus according to the present teachings such as, for non-limiting example, system 200, 300, 400, etc., as described above or the device 900 or 1000, etc., as described below. Other devices or systems in accordance with the present teachings can also be used.
  • A flat target 806 is disposed normal to the path of the laser beam 804. In turn, the laser beam 804 strikes the target 806 as a line of energy 808. Thus, an original (i.e., source) beam of laser energy (not shown) generated within the device 802 has been shaped so as to strike the target 806 as a line-like or narrow, substantially rectangular area 808.
  • Eighth Illustrative Embodiment
  • FIG. 9 depicts a packaged laser device 900 according to another embodiment. The device 900 is illustrative and non-limiting with respect to the present teachings. Other packaged devices can also be configured and/or used according to the present teachings.
  • The device 900 includes a holder tube (i.e., packaging or housing) 902. The holder tube 902 can be formed from any suitable material such as, for non-limiting example, aluminum, stainless steel, etc. Other materials can also be used. The holder tube 902 is configured to protectively house a plurality of elements described hereinafter.
  • The device 900 also includes an edge emitter laser 904. The laser 904 is configured to provide a beam of laser energy. The laser 904 is analogous in operation to the lasers 102, 202, etc. as described above. The laser 904 is supported at one end of the holder tube 902. The device 900 also includes collimation optics 906. The collimation optics 906 are configured to collimate a beam emitted by the laser 904. In one embodiment, the collimation optics 906 are defined by an aspheric lens. Other suitable collimation optics can also be used. The collimation optics 906 are analogous to the collimators 106, 206, etc. as described above. The collimation optics 906 are supported within the holder tube 902.
  • The device 900 includes line generator 908. The line generator 908 is configured to shape the collimated laser beam propagating from the collimation optics 906 into a generally flattened, collimated planar laser beam. In one embodiment, the line generator 908 is defined by an integrated optical element such as, for non-limiting example, the integrated optical elements 310, 410, 510, etc. Other suitable line generators 908 can also be used.
  • The device 900 also includes a slit 910 defined in an end plug 912. Reference is also made to FIG. 9A, which depicts an end elevation view of details of the device 900. The slit 910 is configured to limit width-wise and thickness-wise dimensions of the laser beam emitted from the device 900 during normal operation. In this way, a laser beam having a flattened, generally rectangular cross-sectional energy distribution pattern is provided by the device 900 during normal use. Support elements 914 and 916 are further included within the device 900 so as to fixedly support and space collimation optics 906 and line generator 908. Additionally, an optional spatial filter (not shown) can be included within or adjacent to the slit 910.
  • The device 900 provides an integrated assemblage of elements configured to generate a laser beam having a line-like or rectangular cross-sectional energy distribution of generally constant width and thickness dimensions. The device 900 is applicable, for non-limiting example, in an inkjet printing context to perform drop detection testing of the ink emitter dies. Other suitable applications are also possible.
  • Ninth Illustrative Embodiment
  • FIG. 10 depicts a packaged laser device 1000 according to another embodiment. The device 1000 is illustrative and non-limiting with respect to the present teachings. Other packaged devices can also be configured and/or used according to the present teachings.
  • The device 1000 includes a holder tube (i.e., packaging or housing) 1002. The holder tube 1002 can be formed from any suitable material such as, for non-limiting example, aluminum, stainless steel, etc. Other materials can also be used. The holder tube 1002 is configured to protectively house a plurality of elements described hereinafter.
  • The device 1000 also includes a vertical-cavity surface-emitting laser (VCSEL) 1004. The laser 1004 is configured to provide a beam of laser energy. The laser 1004 is analogous in operation to the lasers 102, 202, etc. as described above. The laser 1004 is supported at one end of the holder tube 1002. The device 1000 also includes optional collimation optics 1006. The collimation optics 1006 are configured to collimate a beam emitted by the laser 1004. In one embodiment, the collimation optics 1006 include a spheric or aspheric lens. Other suitable collimation optics can also be used. The collimation optics 1006 are analogous to the collimators 106, 206, etc. as described above. The collimation optics 1006 is supported within the holder tube 1002 or in VCSEL package.
  • The device 1000 includes a line generator 1008. The line generator 1008 is configured to shape the collimated laser beam propagating from the (optional) collimation optics 1006 into a generally flattened, collimated planar laser beam. In one embodiment, the line generator 1008 is defined by an integrated optical element such as, for non-limiting example, the integrated optical elements 310, 410, 510, etc. Other suitable line generators 1008 can also be used.
  • The device 1000 also includes a slit 1010 defined in an end plug 1012. Reference is also made to FIG. 10A, which depicts an end elevation view of details of the device 1000. The slit 1010 is configured to limit a width-wise dimension and a thickness-wise dimension of the laser beam emitted from the device 1000 during normal operation. In this way, a laser beam having a flattened, rectangular cross-sectional pattern is provided by the device 1000 during normal use. Support elements 1014 and 1016 are further included within the device 1000 so as to fixedly support and space collimation optics 1006 and line generator 1008. Additionally, a spatial filter (not shown) can be optionally included within or adjacent to the slit 1010.
  • The device 1000 provides an integrated assemblage of elements configured to generate a laser beam having a line-like or rectangular cross-sectional energy distribution of generally constant width and thickness dimensions. The device 1000 is applicable, for non-limiting example, in an inkjet printing context to perform drop detection testing of the ink emission nozzles. Other suitable applications are also possible.

Claims (15)

1. An apparatus, comprising:
a line generator configured to shape a collimated laser beam into an expanding planar laser beam, the line generator including at least one planar surface through which the expanding planar laser beam passes; and
a collimator configured to collimate the expanding planar laser beam in at least a fast axis or a slow axis so as to derive a collimated planar laser beam.
2. The apparatus according to claim 1 further comprising:
an emitter configured to provide a laser beam having a Gaussian cross-sectional distribution;
a lens disposed in the path of the laser beam, the lens configured to shape the laser beam into the collimated laser beam.
3. The apparatus according to claim 1, the line generator including a diffraction grating surface.
4. The apparatus according to claim 1 the line generator including a lenticular lens array.
5. The apparatus according to claim 1, the line generator including a Fresnel surface.
6. The apparatus according to claim 1, the collimator including a cylindrical lens.
7. The apparatus according to claim 1, the collimator including a Fresnel cylindrical lens or a Fresnel acylindrical lens.
8. The apparatus according to claim 1, the collimator including a cylindrical lens surface.
9. The apparatus according to claim 1, the collimator including an acylindrical lens surface.
10. The apparatus according to claim 1 further comprising a solid transparent media disposed within the path of the expanding planar laser beam, the solid transparent media configured to support the line generator and the collimator.
11. An optical apparatus, comprising:
a solid-state laser configured to emit a laser beam;
first collimation optics configured to shape the laser beam into a collimated laser beam;
line generator optics configured to shape the collimated laser beam into an expanding planar laser beam, the line generator optics including a planar optical surface through which the expanding planar laser beam passes; and
second collimation optics configured to shape the expanding planar laser beam into a collimated planar laser beam.
12. The optical apparatus according to claim 11, the line generator optics including at least a diffraction grating, diffraction grating surface, a lenticular lens array, a lenticular lens array surface, or a Fresnel surface.
13. The optical apparatus according to claim 11 the second collimation optics including at least a cylindrical lens, a Fresnel cylindrical lens, a cylindrical lens surface, a Fresnel cylindrical lens surface, or an acylindrical lens surface.
14. The optical apparatus according to claim 11 further comprising a spatial filter disposed to filter the collimated planar laser beam.
15. An integrated apparatus; comprising:
a packaging;
a laser emitter supported by the packaging;
collimation optics supported by the packaging and configured to collimate a laser beam emitted by the laser emitter;
line generator optics supported by the packaging and configured to shape the collimated laser beam into a planer laser beam having about a rectangular cross-section; and
a slit supported by the packaging and configured to limit at least a width dimension or a thickness dimension of the planar laser beam as it propagates from the packaging.
US12/418,710 2009-04-06 2009-04-06 Laser line generator Active 2029-06-06 US7821718B1 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
US12/418,710 US7821718B1 (en) 2009-04-06 2009-04-06 Laser line generator

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
US12/418,710 US7821718B1 (en) 2009-04-06 2009-04-06 Laser line generator

Publications (2)

Publication Number Publication Date
US20100254020A1 true US20100254020A1 (en) 2010-10-07
US7821718B1 US7821718B1 (en) 2010-10-26

Family

ID=42825981

Family Applications (1)

Application Number Title Priority Date Filing Date
US12/418,710 Active 2029-06-06 US7821718B1 (en) 2009-04-06 2009-04-06 Laser line generator

Country Status (1)

Country Link
US (1) US7821718B1 (en)

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102402889A (en) * 2011-04-24 2012-04-04 张津 Semiconductor green laser beam expansion device
CN102882121A (en) * 2011-07-14 2013-01-16 亚洲光学股份有限公司 Small-sized laser emitting module
US9322962B1 (en) * 2014-10-31 2016-04-26 Everready Precision Ind. Corp. Structured light generation device
US20160161751A1 (en) * 2013-04-11 2016-06-09 Asphericon Gmbh Refractive beam shaper
US20170038033A1 (en) * 2015-08-07 2017-02-09 Everready Precision Ind. Corp. Method for scaling structured light pattern and optical device using the same
WO2017222558A1 (en) * 2016-06-24 2017-12-28 Isee, Inc. Laser-enhanced visual simultaneous localization and mapping (slam) for mobile devices
US9958687B2 (en) 2014-10-31 2018-05-01 Everready Precision Ind. Corp. Apparatus of structured light generation
CN111665581A (en) * 2020-05-12 2020-09-15 杭州驭光光电科技有限公司 Optical device, projection apparatus including the same, and linear projection method
DE102019111638A1 (en) * 2019-05-06 2020-11-12 Jenoptik Optical Systems Gmbh Optical unit and method for operating an optical unit
CN115113409A (en) * 2022-08-26 2022-09-27 成都莱普科技股份有限公司 Linear flat-top light spot generation system, method and equipment based on Dammann grating
US20230328218A1 (en) * 2022-04-08 2023-10-12 Himax Technologies Limited Structured light projector and three-dimensional image sensing apparatus

Families Citing this family (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US8284500B2 (en) * 2009-06-08 2012-10-09 Ayase Co., Ltd. Laser line-generator and laser line-generator module
US9429742B1 (en) 2011-01-04 2016-08-30 Nlight, Inc. High power laser imaging systems
US8835804B2 (en) 2011-01-04 2014-09-16 Nlight Photonics Corporation Beam homogenizer
US9409255B1 (en) 2011-01-04 2016-08-09 Nlight, Inc. High power laser imaging systems
US10095016B2 (en) 2011-01-04 2018-10-09 Nlight, Inc. High power laser system
TW201249035A (en) * 2011-05-27 2012-12-01 Asia Optical Co Inc Miniaturized laser emitting module
US9720244B1 (en) 2011-09-30 2017-08-01 Nlight, Inc. Intensity distribution management system and method in pixel imaging
US9321349B2 (en) * 2011-12-29 2016-04-26 Intel Corporation Configurable control panels
US9310248B2 (en) 2013-03-14 2016-04-12 Nlight, Inc. Active monitoring of multi-laser systems
KR102099722B1 (en) 2014-02-05 2020-05-18 엔라이트 인크. Single-emitter line beam system
US9907636B2 (en) * 2015-07-01 2018-03-06 3M Innovative Properties Company Curing lights with homogenous light patch

Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5095386A (en) * 1990-05-01 1992-03-10 Charles Lescrenier Optical system for generating lines of light using crossed cylindrical lenses
US5293269A (en) * 1991-05-03 1994-03-08 Mcdonnell Douglas Corporation Aspheric cylindrical lens and method of fabrication
US6016227A (en) * 1998-07-31 2000-01-18 The University Of Tennessee Research Corporation Apparatus and method for producing an improved laser beam
US6845119B2 (en) * 2001-07-23 2005-01-18 Giesecke & Devrient Gmbh Laser illuminating apparatus for illuminating a strip-shaped or linear area
US6991166B2 (en) * 1999-06-07 2006-01-31 Metrologic Instruments, Inc. LED-based planar light illumination and imaging (PLIIM) engine
US7487596B2 (en) * 2004-06-25 2009-02-10 Irwin Industrial Tool Company Laser line projected on an edge of a surface
US7520062B2 (en) * 2005-12-06 2009-04-21 Robert Bosch Tool Corporation Light-plane projecting apparatus and lens
US20090244163A1 (en) * 2008-03-25 2009-10-01 Alexander Govyadinov Drop detection mechanism and a method of use thereof

Patent Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5095386A (en) * 1990-05-01 1992-03-10 Charles Lescrenier Optical system for generating lines of light using crossed cylindrical lenses
US5293269A (en) * 1991-05-03 1994-03-08 Mcdonnell Douglas Corporation Aspheric cylindrical lens and method of fabrication
US6016227A (en) * 1998-07-31 2000-01-18 The University Of Tennessee Research Corporation Apparatus and method for producing an improved laser beam
US6991166B2 (en) * 1999-06-07 2006-01-31 Metrologic Instruments, Inc. LED-based planar light illumination and imaging (PLIIM) engine
US6845119B2 (en) * 2001-07-23 2005-01-18 Giesecke & Devrient Gmbh Laser illuminating apparatus for illuminating a strip-shaped or linear area
US7487596B2 (en) * 2004-06-25 2009-02-10 Irwin Industrial Tool Company Laser line projected on an edge of a surface
US7520062B2 (en) * 2005-12-06 2009-04-21 Robert Bosch Tool Corporation Light-plane projecting apparatus and lens
US20090244163A1 (en) * 2008-03-25 2009-10-01 Alexander Govyadinov Drop detection mechanism and a method of use thereof

Cited By (14)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102402889A (en) * 2011-04-24 2012-04-04 张津 Semiconductor green laser beam expansion device
CN102882121A (en) * 2011-07-14 2013-01-16 亚洲光学股份有限公司 Small-sized laser emitting module
US9547177B2 (en) * 2013-04-11 2017-01-17 Asphericon Gmbh Refractive beam shaper
US20160161751A1 (en) * 2013-04-11 2016-06-09 Asphericon Gmbh Refractive beam shaper
US10133078B2 (en) 2014-10-31 2018-11-20 Everready Precision Ind. Corp. Apparatus of structured light generation
US9958687B2 (en) 2014-10-31 2018-05-01 Everready Precision Ind. Corp. Apparatus of structured light generation
US9322962B1 (en) * 2014-10-31 2016-04-26 Everready Precision Ind. Corp. Structured light generation device
US20170038033A1 (en) * 2015-08-07 2017-02-09 Everready Precision Ind. Corp. Method for scaling structured light pattern and optical device using the same
US9874759B2 (en) * 2015-08-07 2018-01-23 Everready Precision Ind. Corp. Method for scaling structured light pattern and optical device using the same
WO2017222558A1 (en) * 2016-06-24 2017-12-28 Isee, Inc. Laser-enhanced visual simultaneous localization and mapping (slam) for mobile devices
DE102019111638A1 (en) * 2019-05-06 2020-11-12 Jenoptik Optical Systems Gmbh Optical unit and method for operating an optical unit
CN111665581A (en) * 2020-05-12 2020-09-15 杭州驭光光电科技有限公司 Optical device, projection apparatus including the same, and linear projection method
US20230328218A1 (en) * 2022-04-08 2023-10-12 Himax Technologies Limited Structured light projector and three-dimensional image sensing apparatus
CN115113409A (en) * 2022-08-26 2022-09-27 成都莱普科技股份有限公司 Linear flat-top light spot generation system, method and equipment based on Dammann grating

Also Published As

Publication number Publication date
US7821718B1 (en) 2010-10-26

Similar Documents

Publication Publication Date Title
US7821718B1 (en) Laser line generator
US8614853B2 (en) Two-dimensional wavelength-beam-combining of lasers using first-order grating stack
US9720145B2 (en) High brightness multijunction diode stacking
US8602592B2 (en) Diode-laser illuminator with interchangeable modules for changing irradiance and beam dimensions
CN103688426B (en) Pump light arrangement for a disc laser
US20070195850A1 (en) Diode laser array stack
US8220965B2 (en) Laser energy source device and method
RU2015151016A (en) DEVICES, SYSTEMS AND METHODS OF 3D PRINTING
US20230275404A1 (en) Laser system with staircased slow-axis collimators
US9541721B2 (en) Laser device
CN104205530A (en) Semiconductor laser optical device
US20190173255A1 (en) Laser Diode Device and a Projector Using Same
KR20220071965A (en) Hybrid Spectral and Coherent Combined Fiber Laser Amplifier System With Compact Tiled Coherent Optical Monolithic Phased Array
EP3700030B1 (en) Light source device, direct diode laser system, and optical coupling device
US11428520B2 (en) Distance measurement unit and light irradiation device
JP2022527764A (en) Fiber coupling diode laser module and its assembly method
US9608410B2 (en) Surface-emitting light source and laser apparatus
JP2016082219A (en) Semiconductor laser oscillator
WO2021229918A1 (en) Optical module and distance measuring equipment
JP2011501879A (en) Diode laser with beamformer
US8867586B2 (en) Diode laser
JP2021152567A (en) Light source device, projector, and machining device
JP2004518107A (en) Optical distance measuring device
RU134839U1 (en) LASER MARKING DEVICE WITH LASER RADIATION COLLIMATOR
CN210775920U (en) Semiconductor laser emission and coupling module based on novel semiconductor laser chip

Legal Events

Date Code Title Description
AS Assignment

Owner name: HEWLETT-PACKARD DEVELOPMENT COMPANY, L.P., TEXAS

Free format text: ASSIGNMENT OF ASSIGNORS INTEREST;ASSIGNORS:GOVYADINOV, ALEXANDER;SEALS, LENWARD;SIGNING DATES FROM 20090331 TO 20090403;REEL/FRAME:022531/0515

STCF Information on status: patent grant

Free format text: PATENTED CASE

CC Certificate of correction
FPAY Fee payment

Year of fee payment: 4

MAFP Maintenance fee payment

Free format text: PAYMENT OF MAINTENANCE FEE, 8TH YEAR, LARGE ENTITY (ORIGINAL EVENT CODE: M1552)

Year of fee payment: 8

MAFP Maintenance fee payment

Free format text: PAYMENT OF MAINTENANCE FEE, 12TH YEAR, LARGE ENTITY (ORIGINAL EVENT CODE: M1553); ENTITY STATUS OF PATENT OWNER: LARGE ENTITY

Year of fee payment: 12