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    • 3. 发明申请
    • ELLIPSOIDAL MICROCAVITY PLASMA DEVICES AND POWDER BLASTING FORMATION
    • ELLIPSOIDAL微波等离子体装置和粉末喷砂形成
    • US20100072893A1
    • 2010-03-25
    • US12235796
    • 2008-09-23
    • J. Gary EdenSung-Jin ParkSeung Hoon Sung
    • J. Gary EdenSung-Jin ParkSeung Hoon Sung
    • H01J17/49H01J9/24
    • H01J65/046H01J9/241H01J11/18
    • The invention provides microcavity plasma devices and arrays that are formed in layers that also seal the plasma medium, i.e., gas(es) and/or vapors. No separate packaging layers are required and additional packaging can be omitted if it is desirable to do so. A preferred microcavity plasma device includes first and second thin layers that are joined together. A half ellipsoid microcavity or plurality of half ellipsoid microcavities is defined in one or both of the first and second thin layers, and electrodes are arranged with respect to the microcavity to excite a plasma within said microcavities upon application of a predetermined voltage to the electrodes. A method for forming a microcavity plasma device having a plurality of half or full ellipsoid microcavities in one or both of first and second thin layers is also provided by a preferred embodiment. The method includes defining a pattern of protective polymer on the first thin layer. Powder blasting forms half ellipsoid microcavities in the first thin layer. The second thin layer is joined to the first layer. The patterning can be conducted lithographically or can be conduced with a simple screen.
    • 本发明提供了形成为也密封等离子体介质即气体和/或蒸汽的层的微腔等离子体装置和阵列。 不需要单独的包装层,如果要这样做,可以省略额外的包装。 优选的微腔等离子体装置包括连接在一起的第一和第二薄层。 半椭圆形微腔或多个半椭圆形微腔被限定在第一和第二薄层中的一个或两个中,并且相对于微腔布置电极,以在对电极施加预定电压时在所述微腔内激发等离子体。 优选实施例也提供了一种在第一和第二薄层中的一个或两个中形成具有多个半或全椭圆形微腔的微腔等离子体装置的方法。 该方法包括在第一薄层上限定保护性聚合物的图案。 粉末喷射在第一薄层中形成半椭圆形微腔。 第二薄层连接到第一层。 图案化可以光刻地进行,或者可以用简单的屏幕进行。
    • 4. 发明授权
    • Low voltage microcavity plasma device and addressable arrays
    • 低电压微腔等离子体器件和可寻址阵列
    • US07615926B2
    • 2009-11-10
    • US11811892
    • 2007-06-12
    • J. Gary EdenSung-Jin ParkPaul A. TchertchianSeung Hoon Sung
    • J. Gary EdenSung-Jin ParkPaul A. TchertchianSeung Hoon Sung
    • H01J17/49
    • H01J11/12
    • Microcavity plasma devices and arrays of microcavity plasma devices are provided that have a reduced excitation voltage. A trigger electrode disposed proximate to a microcavity reduce the excitation voltage required between first and second electrodes to ignite a plasma in the microcavity when gas(es) or vapor(s) (or combinations thereof) are contained within the microcavity. The invention also provides symmetrical microplasma devices and arrays of microcavity plasma devices for which current waveforms are the same for each half-cycle of the voltage driving waveform. Additionally, the invention also provides devices that have standoff portions and voids that can reduce cross talk. The devices are preferably also used with a trigger electrode.
    • 提供微腔等离子体器件和微腔等离子体器件的阵列,其具有降低的激发电压。 在微腔内包含气体或蒸汽(或其组合)时,靠近微腔设置的触发电极减小了第一和第二电极之间所需的激发电压,以点燃微腔中的等离子体。 本发明还提供对称的微等离子体装置和微腔等离子体装置的阵列,其电流波形对于电压驱动波形的每个半周期是相同的。 此外,本发明还提供了具有能够减少串扰的间隔部分和空隙的装置。 这些装置优选地也与触发电极一起使用。
    • 5. 发明授权
    • Ellipsoidal microcavity plasma devices and powder blasting formation
    • 椭球微腔等离子体装置和粉末爆破形成
    • US08179032B2
    • 2012-05-15
    • US12235796
    • 2008-09-23
    • J. Gary EdenSung-Jin ParkSeung Hoon Sung
    • J. Gary EdenSung-Jin ParkSeung Hoon Sung
    • H01J1/00H01J1/88
    • H01J65/046H01J9/241H01J11/18
    • The invention provides microcavity plasma devices and arrays that are formed in layers that also seal the plasma medium, i.e., gas(es) and/or vapors. No separate packaging layers are required and additional packaging can be omitted if it is desirable to do so. A preferred microcavity plasma device includes first and second thin layers that are joined together. A half ellipsoid microcavity or plurality of half ellipsoid microcavities is defined in one or both of the first and second thin layers, and electrodes are arranged with respect to the microcavity to excite a plasma within said microcavities upon application of a predetermined voltage to the electrodes. A method for forming a microcavity plasma device having a plurality of half or full ellipsoid microcavities in one or both of first and second thin layers is also provided by a preferred embodiment. The method includes defining a pattern of protective polymer on the first thin layer. Powder blasting forms half ellipsoid microcavities in the first thin layer. The second thin layer is joined to the first layer. The patterning can be conducted lithographically or can be conduced with a simple screen.
    • 本发明提供了形成为也密封等离子体介质即气体和/或蒸汽的层的微腔等离子体装置和阵列。 不需要单独的包装层,如果要这样做,可以省略额外的包装。 优选的微腔等离子体装置包括连接在一起的第一和第二薄层。 半椭圆形微腔或多个半椭圆形微腔被限定在第一和第二薄层中的一个或两个中,并且相对于微腔布置电极,以在对电极施加预定电压时在所述微腔内激发等离子体。 优选实施例也提供了一种在第一和第二薄层中的一个或两个中形成具有多个半或全椭圆形微腔的微腔等离子体装置的方法。 该方法包括在第一薄层上限定保护性聚合物的图案。 粉末喷射在第一薄层中形成半椭圆形微腔。 第二薄层连接到第一层。 图案化可以光刻地进行,或者可以用简单的屏幕进行。
    • 6. 发明申请
    • Low voltage microcavity plasma device and addressable arrays
    • 低电压微腔等离子体器件和可寻址阵列
    • US20080129185A1
    • 2008-06-05
    • US11811892
    • 2007-06-12
    • J.Gary EdenSung-Jin ParkPaul A. TchertchianSeung Hoon Sung
    • J.Gary EdenSung-Jin ParkPaul A. TchertchianSeung Hoon Sung
    • H05H1/24
    • H01J11/12
    • Microcavity plasma devices and arrays of microcavity plasma devices are provided that have a reduced excitation voltage. A trigger electrode disposed proximate to a microcavity reduce the excitation voltage required between first and second electrodes to ignite a plasma in the microcavity when gas(es) or vapor(s) (or combinations thereof) are contained within the microcavity. The invention also provides symmetrical microplasma devices and arrays of microcavity plasma devices for which current waveforms are the same for each half-cycle of the voltage driving waveform. Additionally, the invention also provides devices that have standoff portions and voids that can reduce cross talk. The devices are preferably also used with a trigger electrode.
    • 提供微腔等离子体器件和微腔等离子体器件的阵列,其具有降低的激发电压。 在微腔内包含气体或蒸汽(或其组合)时,靠近微腔设置的触发电极减小了第一和第二电极之间所需的激发电压,以点燃微腔中的等离子体。 本发明还提供对称的微等离子体装置和微腔等离子体装置的阵列,其电流波形对于电压驱动波形的每个半周期是相同的。 此外,本发明还提供了具有能够减少串扰的间隔部分和空隙的装置。 这些装置优选地也与触发电极一起使用。
    • 9. 发明授权
    • Microchannel laser having microplasma gain media
    • 具有微质增益介质的微通道激光器
    • US08442091B2
    • 2013-05-14
    • US12682977
    • 2008-10-27
    • Sung-Jin ParkJ. Gary EdenPaoyei ChenPaul A. TchertchianThomas M. Spinka
    • Sung-Jin ParkJ. Gary EdenPaoyei ChenPaul A. TchertchianThomas M. Spinka
    • H01S3/091
    • H01S3/05H01S3/03H01S3/063H01S3/09H01S3/0971
    • The invention provides microchannel lasers having a microplasma gain medium. Lasers of the invention can be formed in semiconductor materials, and can also be formed in polymer materials. In a microlaser of the invention, high density plasmas are produced in microchannels. The microplasma acts as a gain medium with the electrodes sustaining the plasma in the microchannel. Reflectors are used with the microchannel for obtaining optical feedback to obtain lasing in the microplasma gain medium in devices of the invention for a wide range of atomic and molecular species. Several atomic and molecular gain media will produce sufficiently high gain coefficients that reflectors (mirrors) are not necessary. Microlasers of the invention are based on microplasma generation in channels of various geometries. Preferred embodiment microlaser designs can be fabricated in semiconductor materials, such as Si wafers, by standard photolithographic techniques, or in polymers by replica molding.
    • 本发明提供了具有微质增益介质的微通道激光器。 本发明的激光器可以形成在半导体材料中,也可以形成在聚合物材料中。 在本发明的微型激光器中,在微通道中产生高密度等离子体。 微量体作为增益介质,其中电极在微通道中维持等离子体。 反射器与微通道一起使用以获得光学反馈,以在广泛的原子和分子物种的本发明装置中的微量级增益介质中获得激光。 几个原子和分子增益介质将产生足够高的增益系数,反射器(反射镜)不是必需的。 本发明的微型扫描器基于各种几何形状的通道中的微量生成。 优选实施例微激光器设计可以通过标准光刻技术在半导体材料(例如Si晶片)中或通过复制成型制成聚合物。
    • 10. 发明授权
    • Method of making arrays of thin sheet microdischarge devices
    • 制备薄片微放电器件阵列的方法
    • US08221179B2
    • 2012-07-17
    • US11981412
    • 2007-10-31
    • J. Gary EdenSung-Jin ParkClark J. Wagner
    • J. Gary EdenSung-Jin ParkClark J. Wagner
    • H01J17/49
    • H01J17/49H01J1/025H01J9/00H01J9/02H01J25/50H01J61/09H01J61/305H01J61/62H01J63/04H01J65/046
    • The cavity 102 defines an empty volume formed in the insulator 108 has its walls defined by the insulator 108 and may extend through either (or both) the first electrode 106 or the second electrode 104, in which case the first electrode and/or second electrode also define the walls of the cavity 102. The cavity 102 is preferably cylindrical and has a diameter of 0.1 μm-1 mm. More preferably, the diameter ranges from 0.1 μm-500 μm, 1 μm-100 μm, or 100 μm-500 μm. The cavity 102 will be filled with a gas that contacts the cavity walls, fills the entire cavity 102 and is selected for its breakdown voltage or light emission properties at breakdown. Light is produced when the voltage difference between the first electrode 106 and the second electrode 104 creates an electric field sufficiently large to electrically break down the gas (nominally about 104 V-cm). This light escapes from the microcavity 102 through at least one end of the cavity 102.
    • 空腔102限定在绝缘体108中形成的空的体积具有由绝缘体108限定的壁,并且可延伸穿过第一电极106或第二电极104(或两者)中的一个或两者,在这种情况下,第一电极和/或第二电极 还限定空腔102的壁。空腔102优选是圆柱形的并且具有0.1μm-1mm的直径。 更优选的是,直径为0.1μm〜500μm,1μm〜100μm或100μm〜500μm。 空腔102将填充有与空腔壁接触的气体,填充整个空腔102,并且在击穿时选择其击穿电压或发光特性。 当第一电极106和第二电极104之间的电压差产生足够大的电场以电气分解气体(标称约为104V-cm)时产生光。 该光通过空腔102的至少一端从微腔102逸出。