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    • 1. 发明授权
    • Method for determining charged energy states of semiconductor or
insulator materials by using deep level transient spectroscopy, and an
apparatus for carrying out the method
    • 通过使用深层瞬态光谱法确定半导体或绝缘体材料的带电能态的方法,以及用于执行该方法的装置
    • US4571541A
    • 1986-02-18
    • US439226
    • 1982-11-04
    • Gyorgy FerencziJanos BodaFerenc TothPeter HorvathLaszlo BenkovicsLaszlo Dozsa
    • Gyorgy FerencziJanos BodaFerenc TothPeter HorvathLaszlo BenkovicsLaszlo Dozsa
    • G01N27/00G01R31/26G01R31/28H01L21/66
    • G01R31/2831
    • A method for determining charged energy states of a sample of a semiconductor or insulator material by using deep level transient spectroscopy. The method includes the steps of exciting the sample by application of periodical exciting pulses to change the initial charge state, detecting the transient response of the sample when it returns to the thermodynamical balance condition following the termination of each of the excitation pulses, blocking the detection during a blocking period defined as the combined existence of the exciting pulses and of a dead period including the recovery period of the means used for the detection, performing a weighted integration operation on a detected response signal by the application of a symmetrical square wave synchronizing pulse as a weighting function synchronized to the frequency of said exciting pulses, blocking the detection in each of said detecting periods for the duration of a further blocking period which begins in a moment defined between the starting moments of the two exciting pulses immediately preceding and following said detecting period and synchronizing the synchronizing pulses to terminating moments of said dead periods to have a period time which is equal to the period time of said periodical exciting pulses. Apparatus for carrying out the method is also disclosed.
    • 一种通过使用深层瞬态光谱法确定半导体或绝缘体材料样品的带电能态的方法。 该方法包括以下步骤:通过施加周期激励脉冲来激发样品以改变初始电荷状态,当样品在每个激发脉冲终止后返回到热力学平衡条件时检测样品的瞬态响应,阻止检测 在被定义为激励脉冲的组合存在和包括用于检测的装置的恢复周期的死区的阻塞期间中,通过应用对称的方波同步脉冲对检测到的响应信号执行加权积分运算 作为与所述激励脉冲的频率同步的加权函数,在每个所述检测周期内阻止在另一阻塞周期的持续时间内的检测,该进一步的阻塞周期从紧接在所述激励脉冲之前和之后的两个激励脉冲的起始时刻之间限定的时刻开始 检测周期并同步同步pu 导致所述死区的终止时刻具有等于所述周期激励脉冲的周期时间的周期时间。 还公开了用于执行该方法的装置。
    • 3. 发明授权
    • Method and apparatus for measuring minority carrier lifetime in
semiconductor materials
    • 测量半导体材料中少数载流子寿命的方法和装置
    • US5406214A
    • 1995-04-11
    • US808671
    • 1991-12-16
    • Janos BodaGyorgy FerencziPeter HorvathZoltan MirkTibor Pavelka
    • Janos BodaGyorgy FerencziPeter HorvathZoltan MirkTibor Pavelka
    • G01N22/00G01R31/265G01R31/26G01R27/06
    • G01N22/00G01R31/2656
    • A contactless apparatus for measuring contaminants in a semiconductor specimen (24) includes a tunable microwave generator (26) coupled by a coaxial cable (36) to a tuned narrowband microstrip antenna (38) that defines a through hole (72). The antenna is placed in near field relationship to the specimen to direct microwave energy toward a first specimen surface (44). This proximity provides a substantially more powerful microwave field than prior art systems, and the specimen comprises an impedance termination for the microwave path that includes the microwave generator and antenna, thereby rendering system measurements substantially immune to mechanical vibration of the specimen. A pulsed laser (42) directs optical energy through the antenna through hole toward the first specimen surface (44). The optical energy generates minority carriers within the specimen that begin to recombine upon cessation of each pulse. Minority lifetime decay affects microwave energy reflecting from freed holes and electrons in the specimen, which energy is coupled from the antenna to a detector (46) and preferably a computer system (48) that controls the system and provides signal processing of the detector output.
    • 用于测量半导体样品(24)中的污染物的非接触式设备包括可调谐微波发生器(26),其通过同轴电缆(36)耦合到限定通孔(72)的调谐窄带微带天线(38)。 将天线放置成与样品的近场关系,以将微波能量引向第一样品表面(44)。 该接近度提供了比现有技术系统更强大的微波场,并且样本包括用于包括微波发生器和天线的微波路径的阻抗终端,从而使得系统测量基本上不受样本的机械振动的影响。 脉冲激光器(42)将光能通过天线通孔朝向第一样品表面(44)引导。 光能在样品中产生少量载体,在每个脉冲停止时开始复合。 少数生命周期衰减影响从样品中释放的空穴和电子反射的微波能量,该能量从天线耦合到检测器(46),优选地控制系统并提供检测器输出的信号处理的计算机系统(48)。
    • 4. 发明授权
    • Method and apparatus for determining the layer thickness of
semiconductor layer structures
    • 用于确定半导体层结构层厚度的方法和装置
    • US4995939A
    • 1991-02-26
    • US301889
    • 1989-02-08
    • Gyorgy FerencziKatalin ErdelyiMaria SomogyiJanos BodaGyorgy FuleGabor Aszodi
    • Gyorgy FerencziKatalin ErdelyiMaria SomogyiJanos BodaGyorgy FuleGabor Aszodi
    • H01L21/306G01B7/06G01N27/42
    • G01B7/06G01N27/42
    • In a process for determining the layer thickness of semiconductor layer structures, a sample of a multilayer semi-conductor (4) is placed in contact with an electrolyte (2) then subjected to anodic etching during which the depth of etching is determined by integration of the current. During etching, the sample (4) is also excited by an electric signal and the real component of the admittance and hence the conductance of the probe at the frequency of excitation is determined, the extreme values of this component are analyzed, and the values of the depth of etching corresponding to these extremes, which characterize the junctions between the layers of the sample (4) tested, are determined. The installation for implementing the procedure contains a cell (1) filled with electrolyte (2) in which is immersed a graphite electrode (5), a saturated calomel electrode (6), and a platinum electrode (7) surrounding the surface of the sample (4) subjected to etching, electrodes (8,9) neither of which touch the surface of the sample (4) subjected to etching, a potentiostat (13) which is connected to the calomel electrode (6) and the direct current source (12), the current integrator (14), which receives the etching current intensity signal, a generator (15) which emits a periodic signal between the sample (14) and the metal electrode, and the measurement element (16) for measuring the conductance of the sample (4).
    • PCT No.PCT / HU88 / 00030 Sec。 371日期:1989年2月8日 102(e)日期1989年2月8日PCT提交1988年5月4日PCT公布。 第WO88 / 09053号公报 日期:1988年11月17日。在确定半导体层结构的层厚度的方法中,将多层半导体(4)的样品放置成与电解质(2)接触,然后进行阳极蚀刻, 的蚀刻由电流的积分确定。 在蚀刻期间,样品(4)也被电信号激发,确定激励频率下的导纳的实际分量,从而确定探针的电导,分析该分量的极值, 确定对应于这些极限的蚀刻深度,其表征测试的样品(4)的层之间的结。 用于实施该方法的装置包含一个填充有电解质(2)的电池(1),其中浸入石墨电极(5),饱和甘汞电极(6)和围绕该样品表面的铂电极(7) (4)进行蚀刻,两者都不接触经受蚀刻的样品(4)的表面的电极(8,9),与甘汞电极(6)和直流电源(6)连接的恒电位仪(13) 12),接收蚀刻电流强度信号的电流积分器(14),在样品(14)和金属电极之间发射周期性信号的发生器(15)和用于测量电导率的测量元件(16) 的样品(4)。
    • 5. 发明授权
    • Turbulent heat exchanger
    • 湍流换热器
    • US4830102A
    • 1989-05-16
    • US70672
    • 1987-07-02
    • Arpad BakayJanos BodaLaszlo ForgoIstvan PappGyula KovacsKaroly Laszlo
    • Arpad BakayJanos BodaLaszlo ForgoIstvan PappGyula KovacsKaroly Laszlo
    • F28F13/06F28D7/00F28D9/02F28F1/32F28F13/12
    • F28F13/12F28F1/325Y10S165/502
    • A heat exchanger having a plurality of parallel pipes arranged in lines and strips of fin plates fixed to the pipes perpendicularly to the lengths thereof. Turbulence-forming structures are cut out of the fin plates and are bent up at 90.degree. with respect to the planes of the plates, such structures functioning as fin plate spacers and as baffles to direct a fluid medium of inferior heat transfer coefficient which flows in a direction parallel to the planes of the finned plates and perpendicularly to the pipes. The pipes are adapted to conduct a fluid medium of superior heat transfer coefficient. The turbulence-forming structures are disposed in lines on each side of the lines of pipes and in rows which are substantially tangential to the opposite sides of the pipes. The heat exchanger may have a plurality of lines of pipes spaced equally transversely from each other and transvetsely of the direction of flow of the fluid medium of inferior heat transfer coefficient. Further turbulence-forming structures may be disposed along the center line between the successive lines of pipes.
    • 一种热交换器,具有多个平行的管道,排列成与其长度垂直的管道和翅片板条。 湍流形成结构从翅片板切出,并相对于板的平面向上弯曲90度,这种结构用作翅片板间隔件和挡板,以引导传热系数差的流体介质 平行于翅片板的平面并垂直于管道的方向。 管道适于传导具有优良传热系数的流体介质。 湍流形成结构在管道的每一侧上排成一行,并且与管的相对侧基本上相切地排成一排。 热交换器可以具有彼此横向间隔开的多条管线,并且传输具有差的传热系数的流体介质的流动方向。 另外的湍流形成结构可以沿着连续的管道线之间的中心线设置。