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    • 1. 发明授权
    • Method for minimizing sample damage during the ablation of material using a focused ultrashort pulsed laser beam
    • 使用聚焦超短脉冲激光束消融材料期间样品损伤最小化的方法
    • US07649153B2
    • 2010-01-19
    • US09933461
    • 2001-08-20
    • Richard Alan HaightPeter P. LongoDaniel Peter MorrisAlfred Wagner
    • Richard Alan HaightPeter P. LongoDaniel Peter MorrisAlfred Wagner
    • B23K26/36B23K26/06
    • A61B18/20A61B18/203A61B18/26A61B2018/00577A61B2018/00625A61F9/00814A61F9/0084A61F2009/00863B23K26/0624B23K26/066B23K26/361B23K26/362B23K26/40B23K26/402B23K2103/30B23K2103/50G03F1/72
    • In one aspect the invention provides a method for laser induced breakdown of a material with a pulsed laser beam where the material is characterized by a relationship of fluence breakdown threshold (Fth) versus laser beam pulse width (T) that exhibits an abrupt, rapid, and distinct change or at least a clearly detectable and distinct change in slope at a predetermined laser pulse width value. The method comprises generating a beam of laser pulses in which each pulse has a pulse width equal to or less than the predetermined laser pulse width value. The beam is focused above the surface of a material where laser induced breakdown is desired. The region of least confusion (minimum beam waist or average spot size) is above the surface of the material in which laser induced breakdown is desired since the intensity of the beam falls off in the forward direction, preferably the region of the beam at or within the surface is between the region of least confusion and sufficient to remove material and the minimum intensity necessary for laser induced breakdown of the material to be removed, most preferably the region of minimum intensity is disposed at the surface of the material to be removed. The beam may be used in combination with a mask in the beam path. The beam or mask may be moved in the x, y, and Z directions to produce desired features. The technique can produce features smaller than the spot size and Rayleigh range due to enhanced damage threshold accuracy in the short pulse regime.
    • 在一个方面,本发明提供了一种用于脉冲激光束的材料的激光诱导击穿的方法,其中材料的特征在于注射击穿阈值(Fth)与激光束脉冲宽度(T)的关系,其显示突然,快速, 并且在预定的激光脉冲宽度值处具有明显的变化或至少清楚可检测和明显的斜率变化。 该方法包括生成激光脉冲束,其中每个脉冲具有等于或小于预定激光脉冲宽度值的脉冲宽度。 光束聚焦在需要激光诱发击穿的材料的表面之上。 最小混乱(最小光束腰部或平均光点尺寸)的区域高于激光诱发击穿所需的材料的表面,因为光束的强度在向前方向上脱落,优选地在波束的或在其内的区域 表面处于最少混淆的区域之间并且足以去除材料并且要被去除的材料的激光诱发击穿所需的最小强度,最优选地,最小强度的区域设置在要去除的材料的表面上。 光束可以与光束路径中的掩模组合使用。 光束或掩模可以在x,y和z方向上移动以产生期望的特征。 该技术可以产生小于点尺寸和瑞利范围的特征,这是由于在短脉冲状态下增强的损伤阈值精度。
    • 2. 发明授权
    • Method for minimizing sample damage during the ablation of a first biological material disposed on a second biological material using a focused ultrashort pulsed laser beam wherein the slope of fluence breakdown is a function of the pulse width
    • 使用聚焦的超短脉冲激光束在布置在第二生物材料上的第一生物材料的烧蚀期间使样品损伤最小化的方法,其中注量分数的斜率是脉冲宽度的函数
    • US08389890B2
    • 2013-03-05
    • US12545216
    • 2009-08-21
    • Richard Alan HaightPeter P. LongoDaniel Peter MorrisAlfred Wagner
    • Richard Alan HaightPeter P. LongoDaniel Peter MorrisAlfred Wagner
    • B23K26/36B23K26/06
    • A61B18/20A61B18/203A61B18/26A61B2018/00577A61B2018/00625A61F9/00814A61F9/0084A61F2009/00863B23K26/0624B23K26/066B23K26/361B23K26/362B23K26/40B23K26/402B23K2103/30B23K2103/50G03F1/72
    • In one aspect the invention provides a method for laser induced breakdown of a material with a pulsed laser beam where the material is characterized by a relationship of fluence breakdown threshold (Fth) versus laser beam pulse width (T) that exhibits an abrupt, rapid, and distinct change or at least a clearly detectable and distinct change in slope at a predetermined laser pulse width value. The method comprises generating a beam of laser pulses in which each pulse has a pulse width equal to or less than the predetermined laser pulse width value. The beam is focused above the surface of a material where laser induced breakdown is desired. The region of least confusion (minimum beam waist or average spot size) is above the surface of the material in which laser induced breakdown is desired since the intensity of the beam falls off in the forward direction, preferably the region of the beam at or within the surface is between the region of least confusion and sufficient to remove material and the minimum intensity necessary for laser induced breakdown of the material to be removed, most preferably the region of minimum intensity is disposed at the surface of the material to be removed. The beam may be used in combination with a mask in the beam path. The beam or mask may be moved in the x, y, and Z directions to produce desired features. The technique can produce features smaller than the spot size and Rayleigh range due to enhanced damage threshold accuracy in the short pulse regime.
    • 在一个方面,本发明提供了一种用于脉冲激光束的材料的激光诱导击穿的方法,其中材料的特征在于注射击穿阈值(Fth)与激光束脉冲宽度(T)的关系,其显示突然,快速, 并且在预定的激光脉冲宽度值处具有明显的变化或至少清楚可检测和明显的斜率变化。 该方法包括生成激光脉冲束,其中每个脉冲具有等于或小于预定激光脉冲宽度值的脉冲宽度。 光束聚焦在需要激光诱发击穿的材料的表面之上。 最小混乱(最小光束腰部或平均光点尺寸)的区域高于激光诱发击穿所需的材料的表面,因为光束的强度在向前方向上脱落,优选地在波束的或在其内的区域 表面处于最少混淆的区域之间并且足以去除材料并且要被去除的材料的激光诱发击穿所需的最小强度,最优选地,最小强度的区域设置在要去除的材料的表面上。 光束可以与光束路径中的掩模组合使用。 光束或掩模可以在x,y和z方向上移动以产生期望的特征。 该技术可以产生小于点尺寸和瑞利范围的特征,这是由于在短脉冲状态下增强的损伤阈值精度。
    • 3. 发明申请
    • METHOD FOR MINIMIZING SAMPLE DAMAGE DURING THE ABLATION OF MATERIAL USING A FOCUSED ULTRASHORT PULSED LASER BEAM WHEREIN THE SLOPE OF FLUENCE BREAKDOWN IS A FUNCTION OF THE PULSE WIDTH
    • 在使用聚焦超声波脉冲激光束的材料消除期间最小化样品损伤的方法在流动断裂的斜率是脉冲宽度的函数
    • US20100006550A1
    • 2010-01-14
    • US12545216
    • 2009-08-21
    • Richard Alan HaightPeter P. LongoDaniel Peter MorrisAlfred Wagner
    • Richard Alan HaightPeter P. LongoDaniel Peter MorrisAlfred Wagner
    • B23K26/00
    • A61B18/20A61B18/203A61B18/26A61B2018/00577A61B2018/00625A61F9/00814A61F9/0084A61F2009/00863B23K26/0624B23K26/066B23K26/361B23K26/362B23K26/40B23K26/402B23K2103/30B23K2103/50G03F1/72
    • In one aspect the invention provides a method for laser induced breakdown of a material with a pulsed laser beam where the material is characterized by a relationship of fluence breakdown threshold (Fth) versus laser beam pulse width (T) that exhibits an abrupt, rapid, and distinct change or at least a clearly detectable and distinct change in slope at a predetermined laser pulse width value. The method comprises generating a beam of laser pulses in which each pulse has a pulse width equal to or less than the predetermined laser pulse width value. The beam is focused above the surface of a material where laser induced breakdown is desired. The region of least confusion (minimum beam waist or average spot size) is above the surface of the material in which laser induced breakdown is desired since the intensity of the beam falls off in the forward direction, preferably the region of the beam at or within the surface is between the region of least confusion and sufficient to remove material and the minimum intensity necessary for laser induced breakdown of the material to be removed, most preferably the region of minimum intensity is disposed at the surface of the material to be removed. The beam may be used in combination with a mask in the beam path. The beam or mask may be moved in the x, y, and Z directions to produce desired features. The technique can produce features smaller than the spot size and Rayleigh range due to enhanced damage threshold accuracy in the short pulse regime.
    • 在一个方面,本发明提供了一种用于脉冲激光束的材料的激光诱导击穿的方法,其中材料的特征在于注射击穿阈值(Fth)与激光束脉冲宽度(T)的关系,其显示突然,快速, 并且在预定的激光脉冲宽度值处具有明显的变化或至少清楚可检测和明显的斜率变化。 该方法包括生成激光脉冲束,其中每个脉冲具有等于或小于预定激光脉冲宽度值的脉冲宽度。 光束聚焦在需要激光诱发击穿的材料的表面之上。 最小混乱(最小光束腰部或平均光点尺寸)的区域高于激光诱发击穿所需的材料的表面,因为光束的强度在向前方向上脱落,优选地在波束的或在其内的区域 表面处于最少混淆的区域之间并且足以去除材料并且要被去除的材料的激光诱发击穿所需的最小强度,最优选地,最小强度的区域设置在要去除的材料的表面上。 光束可以与光束路径中的掩模组合使用。 光束或掩模可以在x,y和z方向上移动以产生期望的特征。 该技术可以产生小于点尺寸和瑞利范围的特征,这是由于在短脉冲状态下增强的损伤阈值精度。
    • 4. 发明授权
    • Method for minimizing sample damage during the ablation of material using a focused ultrashort pulsed beam
    • 使用聚焦超短脉冲光束在材料消融期间最小化样品损伤的方法
    • US06333485B1
    • 2001-12-25
    • US09210226
    • 1998-12-11
    • Richard Alan HaightPeter P. LongoDaniel Peter MorrisAlfred Wagner
    • Richard Alan HaightPeter P. LongoDaniel Peter MorrisAlfred Wagner
    • B23K2602
    • G03F1/72A61B18/26B23K26/0624B23K26/066B23K26/361B23K26/40B23K2103/30B23K2103/50Y10S438/94
    • In one aspect the invention provides a method for laser induced breakdown of a material with a pulsed laser beam where the material is characterized by a relationship of fluence breakdown threshold (Fth) versus laser beam pulse width (T) that exhibits an abrupt, rapid, and distinct change or at least a clearly detectable and distinct change in slope at a predetermined laser pulse width value. The method comprises generating a beam of laser pulses in which each pulse has a pulse width equal to or less than the predetermined laser pulse width value. The beam is focused above the surface of a material where laser induced breakdown is desired. The region of least confusion (minimum beam waist or average spot size) is above the surface of the material in which laser induced breakdown is desired since the intensity of the beam falls off in the forward direction, preferably the region of the beam at or within the surface is between the region of least confusion and sufficient to remove material and the minimum intensity necessary for laser induced breakdown of the material to be removed, most preferably the region of minimum intensity is disposed at the surface of the material to be removed. The beam may be used in combination with a mask in the beam path. The beam or mask may be moved in the x, y, and Z directions to produce desired features. The technique can produce features smaller than the spot size and Rayleigh range due to enhanced damage threshold accuracy in the short pulse regime.
    • 在一个方面,本发明提供了一种用于脉冲激光束的材料的激光诱导击穿的方法,其中材料的特征在于注射击穿阈值(Fth)与激光束脉冲宽度(T)的关系,其显示突然,快速, 并且在预定的激光脉冲宽度值处具有明显的变化或至少清楚可检测和明显的斜率变化。 该方法包括生成激光脉冲束,其中每个脉冲具有等于或小于预定激光脉冲宽度值的脉冲宽度。 光束聚焦在需要激光诱发击穿的材料的表面之上。 最小混乱(最小光束腰部或平均光点尺寸)的区域高于激光诱发击穿所需的材料的表面,因为光束的强度在向前方向上脱落,优选地在波束的或在其内的区域 表面处于最少混淆的区域之间并且足以去除材料并且要被去除的材料的激光诱发击穿所需的最小强度,最优选地,最小强度的区域设置在要去除的材料的表面上。 光束可以与光束路径中的掩模组合使用。 光束或掩模可以在x,y和z方向上移动以产生期望的特征。 该技术可以产生小于点尺寸和瑞利范围的特征,这是由于在短脉冲状态下增强的损伤阈值精度。
    • 7. 发明授权
    • Organic light emitting diodes having transparent cathode structures
    • 具有透明阴极结构的有机发光二极管
    • US5739545A
    • 1998-04-14
    • US794072
    • 1997-02-04
    • Supratik GuhaRichard Alan HaightJoseph M. KarasinskiRonald R. Troutman
    • Supratik GuhaRichard Alan HaightJoseph M. KarasinskiRonald R. Troutman
    • H01L51/50H01L51/52H05B33/12H05B33/14H05B33/22H05B33/26H01L35/24H01L51/00
    • H01L51/5234H01L2251/5323
    • Organic light emitting diodes having a transparent cathode structure is disclosed. The structure consists of a low work function metal in direct contact with the electron transport layer of the OLED covered by a layer of a wide bandgap semiconductor. Calcium is the preferred metal because of its relatively high optical transmissivity for a metal and because of its proven ability to form a good electron injecting contact to organic materials. ZnSe, ZnS or an alloy of these materials are the preferred semiconductors because of their good conductivity parallel to the direction of light emission, their ability to protect the underlying low work function metal and organic films and their transparency to the emitted light. Arrays of these diodes, appropriately wired, can be used to make a self-emissive display. When fabricated on a transparent substrate, such a display is at least partially transparent making it useful for heads-up display applications in airplanes and automobiles. Such a display can also be fabricated on an opaque substrate, such as silicon, in which previously fabricated devices and circuits can be used to drive the display.
    • 公开了具有透明阴极结构的有机发光二极管。 该结构由与宽带隙半导体层覆盖的OLED的电子传输层直接接触的低功函数金属组成。 由于金属具有相对较高的透光率,因此,由于已证明能够与有机材料形成良好的电子注入接触,钙是优选的金属。 ZnSe,ZnS或这些材料的合金是优选的半导体,因为它们具有与光发射方向平行的良好导电性,它们保护下层低功函数金属和有机膜的能力及其对发射光的透明度。 这些二极管的数组,适当连接,可用于进行自发光显示。 当在透明基板上制造时,这种显示器至少部分透明,使其对于在飞机和汽车中的单机显示应用是有用的。 这种显示器也可以在诸如硅的不透明衬底上制造,其中可以使用先前制造的器件和电路来驱动显示器。
    • 9. 发明授权
    • Hybrid organic-inorganic semiconductor light emitting diodes
    • 混合有机 - 无机半导体发光二极管
    • US5895932A
    • 1999-04-20
    • US811990
    • 1997-03-05
    • Nestor A. Bojarczuk, Jr.Supratik GuhaRichard Alan Haight
    • Nestor A. Bojarczuk, Jr.Supratik GuhaRichard Alan Haight
    • H01L33/08H01L33/50H01L51/00H01L51/30H01L51/50H01L33/00
    • H01L33/502H01L51/5036H01L27/153H01L33/08H01L51/0062H01L51/0077H01L51/0081
    • This invention provides a novel hybrid organic-inorganic semiconductor light emitting diode. The device consists of an electroluminescent layer and a photoluminescent layer. The electroluminescent layer is an inorganic GaN light emitting diode structure that is electroluminescent in the blue or ultraviolet (uv) region of the electromagnetic spectrum when the device is operated. The photoluminescent layer is a photoluminescent organic thin film such as tris-(8-hydroxyquinoline) Al, Alq3, deposited onto the GaN LED and which has a high photoluminescence efficiency. The uv emission from the electroluminescent region excites the Alq3 which photoluminesces in the green. Such a photoconversion results in a light emitting diode that operates in the green (in the visible range). Other colors such as blue or red may be obtained by appropriately doping the Alq3. Furthermore, other luminescent organics in addition to Alq3 may be used to directly convert the uv or blue to other wavelengths of interest. The invention provides the benefits of simplicity and ease of fabrication, since a complete redesign of the structure is not necessary to change emission wavelength, and the possibility for making displays by spatially varying the deposition of the emissive layer.
    • 本发明提供一种新颖的混合有机 - 无机半导体发光二极管。 该器件由电致发光层和光致发光层组成。 电致发光层是当器件工作时在电磁光谱的蓝色或紫外(uv)区域中电致发光的无机GaN发光二极管结构。 光致发光层是沉积在GaN LED上的具有高光致发光效率的光致发光有机薄膜,例如三(8-羟基喹啉)Al,Alq 3。 来自电致发光区域的紫外发射激发了绿色光致发光的Alq3。 这种光转换导致以绿色(在可见光范围内)工作的发光二极管。 可以通过适当掺杂Alq3来获得其它颜色,如蓝色或红色。 此外,可以使用除Alq3之外的其它发光有机物,以将紫外或蓝光直接转换成感兴趣的其它波长。 本发明提供了简单和易于制造的优点,因为结构的完全重新设计不需要改变发射波长,以及通过空间上改变发光层的沉积来制造显示的可能性。