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    • 1. 发明申请
    • LIGHT DRIVEN LIQUID CRYSTAL ELASTOMER ACTUATOR
    • 轻型液晶弹性体激光器
    • WO2014082662A1
    • 2014-06-05
    • PCT/EP2012/073749
    • 2012-11-27
    • CNR - CONSIGLIO NAZIONALE DELLE RICERCHEISTITUTO ITALIANO DI TECNOLOGIA
    • WIERSMA, Diederik SyboltPARMEGGIANI, CamillaGOMEZ-LAVOCAT, Jean-ChristopheVYNCK, Kevin
    • F03G7/00B81B3/00
    • B81B3/0029B81B2201/038F03G6/00F03G7/005G02B26/004G02F1/133362Y02E10/46Y10S901/01
    • Liquid crystal elastomer actuator (1) apt to move in a fluid, wherein the actuator includes a body (10) having a dimension comprised between 100 nm and 800 μιη so as to be considered a body having a low Reynolds number. The body (10) comprises: at least a first (2;2a;2b; 20) and a second (3;2c;2d; 30) spatially separated volumes, the first and second volume of the body both comprising a liquid crystal elastomer. The first volume is doped with a first photoactive doping substance apt to absorb electromagnetic radiation at a first wavelength, and the second volume is doped with a second photoactive doping substance apt to absorb electromagnetic radiation at a second wavelength. The first and second volumes are apt to change shape as a consequence of the light absorption at first or second wavelength, so that in the body a first (2j;20j) and a second joint (3j;30j) are defined. Moreover, a first absorbance of the first volume at a given wavelength is different than a second absorbance of the second volume at said given wavelength, the first and second absorbance are measured in the same time interval.
    • 易于在流体中移动的液晶弹性体致动器(1),其中致动器包括具有100nm和800μm之间的尺寸的主体(10) 以便被认为是具有低雷诺数的身体。 主体(10)包括:至少第一(2; 2a; 2b; 20)和第二(3; 2c; 2d; 30)空间分离的体积,主体的第一和第二体积都包括液晶弹性体 。 掺杂第一体积的第一光活性掺杂物质,其倾向于吸收第一波长的电磁辐射,第二体积掺杂有适于吸收第二波长的电磁辐射的第二光活性掺杂物质。 第一和第二体积由于在第一或第二波长处的光吸收而易于改变形状,使得在体内限定了第一(2j; 20j)和第二接头(3j; 30j)。 此外,在给定波长处的第一体积的第一吸光度与所述给定波长处的第二体积的第二吸光度不同,在相同的时间间隔中测量第一和第二吸光度。
    • 2. 发明申请
    • APPARATUS FOR DETERMINING MYOCARDIUM MARTIAL ACCUMULATION BY ANALYSING MAGNETIC RESONANCE IMAGES
    • 用于通过分析磁共振图像确定心肌梗塞累积的装置
    • WO2006134430A2
    • 2006-12-21
    • PCT/IB2006/000880
    • 2006-04-13
    • CNR CONSIGLIO NAZIONALE DELLE RICERCHELANDINI, LuigiPOSITANO, VicenzoPEPE, AlessiaSANTARELLI, Filomena, MariaLOMBARDI, MassimoBENASSI, AntonioL'ABBATE, Antonio
    • LANDINI, LuigiPOSITANO, VicenzoPEPE, AlessiaSANTARELLI, Filomena, MariaLOMBARDI, MassimoBENASSI, AntonioL'ABBATE, Antonio
    • A61B5/055G01N24/08G01R33/50G01R33/5608G01R33/56509
    • An apparatus for analyzing of the distribution of iron content in determined anatomic regions, in particular in the heart, of thalassemic patients subject to many blood transfusion and for which martial accumulation should be monitored. In particular, the apparatus provides magnetic resonance means adapted to measure a succession of images (10), (20, 30), for example at the left ventricle of the myocardium, for different echo times (TE) . More in detail, each succession of images (10) , (20, 30) is taken at a determined height of the heart (50) . For example, by scanning a plurality section of the left ventricle (51) of a patient at a plane α for different echo times (TE) a first succession of images (10) is obtained. Then by of suitable contour tracking means the image is defined so that the contours of the more relevant parts is highlighted. Each image is then computed by means of known algorithms in order to determine the values of the brightness (S) of its pixels. Then on each image (10) of the series an area of analysis (11) assimilated to a corona is defined between an outer contour (13) and an inner contour (14) . The area (11) is then split into different portions, for example four equiangular sectors (15) . For each field (15) of the image (10) it is possible to obtain on a diagram ;a point of coordinates (S, TE) . Repeating the step for different echo times it is possible then to obtain by interpolation a relative brightness decay curve.
    • 用于分析确定的解剖区域,特别是心脏中的铁含量分布的设备,其需要监测许多输血的thalassemic患者,并且应该监测其中的军情积累。 具体地,该装置提供适于在不同回波时间(TE)下测量例如心肌左心室的连续图像(10),(20,30)的磁共振装置。 更详细地,在心脏(50)的确定的高度处拍摄每个连续的图像(10),(20,30)。 例如,通过在不同回波时间(TE)的平面a处扫描患者的左心室(51)的多个部分,获得第一序列图像(10)。 然后通过适当的轮廓跟踪意味着定义图像,使得更相关部分的轮廓被突出显示。 然后通过已知算法计算每个图像,以便确定其像素的亮度(S)的值。 然后,在该系列的每个图像(10)上,在外部轮廓(13)和内部轮廓(14)之间限定了被分解为电晕的分析区域(11)。 然后将区域(11)分成不同的部分,例如四个等角扇区(15)。 对于图像(10)的每个场(15),可以在图上获得坐标点(S,TE)。 对于不同回波次数重复步骤,可以通过插值获得相对亮度衰减曲线。
    • 3. 发明申请
    • METHOD AND APPARATUS FOR INTRODUCING SAMPLES OF GAS AT CONTROLLED PRESSURE IN A GAS CHROMATOGRAPH
    • 气体色谱法中控制压力气体样品介绍的方法与装置
    • WO2006051354A1
    • 2006-05-18
    • PCT/IB2005/001568
    • 2005-06-03
    • CNR CONSIGLIO NAZIONALE DELLE RICERCHECAPRAI, Antonio
    • CAPRAI, Antonio
    • G01N30/32
    • G01N30/32G01N30/16G01N30/466G01N30/66G01N2030/025G01N2030/322G01N2030/625G01N2030/626
    • Apparatus for analysing a gas sample comprising a variable volume chamber (8) in fluodynamic connection through a line (21-22) with a sample holding container (30), in which the gas sample is contained, and through a line (11-19) with a plurality of gaschromatographic instruments, for example two (51, 52). These instruments carry out the quantitative and qualitative analysis of the gas sample according to known techniques. Preliminarily, by vacuum pumps (60), the line (11-23) and the variable volume chamber (8) are vacuumed. Then valves (41, 43, 45) are closed in order to exclude the portions of line set between valves (41, 43) and six-way valves (75, 76) respectively, and a delivery duct (23) of the pump (65), which is the general pumping means of the line. Since the variable volume chamber (8) is under vacuum when it is connected to the sample holding container (30), it attracts a certain quantity of gas sample inside. The pressure of the chamber (8), and then of the sample holding container (30), are monitored instantly by a pressure sensor (25), for example an analogic reader (35) . Once chosen the column (51, 52) that can be used for carrying out the qualitative and quantitative analysis of the gas sample, the corresponding valve (41, 43) is open. Then, starting from a known volume and pressure, the gas sample is compressed, or expanded, changing the volume of the chamber (8), in order to bring the pressure of the gas same within a predetermined range of values for which the response of the detector (70, 71) is linear.
    • 一种用于分析气体样品的装置,包括通过具有样品保持容器(30)的管线(21-22)的流体动力学连接的可变容积室(8),其中容纳气体样品,并且通过管线(11-19 )与多个气相色谱仪器,例如两个(51,52)。 这些仪器根据已知技术对气体样品进行定量和定性分析。 最初,通过真空泵(60),线(11-23)和可变容积室(8)被抽真空。 然后关闭阀门(41,43,45),以分别排除阀门(41,43)和六通阀(75,76)之间的管路部分和泵的输送管道(23) 65),这是线路的一般泵送装置。 由于可变容积室(8)在与样品保持容器(30)连接时处于真空状态,因此吸入一定量的气体样品。 通过压力传感器(25),例如模拟读取器(35)立即监测腔室(8)的压力和样品保持容器(30)的压力。 一旦选择了可用于对气体样品进行定性和定量分析的柱(51,52),则相应的阀(41,43)打开。 然后,从已知的体积和压力开始,气体样品被压缩或膨胀以改变腔室(8)的体积,以便使气体的压力相同于预定范围的值, 检测器(70,71)是线性的。
    • 5. 发明申请
    • FREQUENCY COMB SPECTROSCOPY APPARATUS AND METHOD OF FREQUENCY COMB SPECTROSCOPY
    • 频率合成光谱仪和频率谱分析方法
    • WO2014102572A1
    • 2014-07-03
    • PCT/IB2012/057796
    • 2012-12-28
    • CNR - CONSIGLIO NAZIONALE DELLE RICERCHE
    • GAGLIARDI, GianlucaAVINO, SaverioGIORGINI, AntonioDE NATALE, Paolo
    • G01N21/39G01N21/77G01J3/02G01J3/433
    • G01N21/39G01J3/02G01J3/0218G01J3/28G01J3/2803G01J2003/4332G01N2021/391G01N2021/399G01N2201/06113G01N2201/08
    • The present invention relates to a method and an apparatus to perform frequency comb spectroscopy. The method includes: -Arranging a waveguide optical cavity (3) having a plurality of cavity mode frequencies with a cavity mode frequency spacing (FSR), said waveguide optical cavity being dispersive so that the frequency spacing of the cavity modes is wavelength dependent; -Arranging a sample (S) with respect to the waveguide optical cavity (3) so that the sample is capable of absorbing light travelling into the waveguide optical cavity; -Coupling pulsed light coming from a light source (1) into the waveguide optical cavity (3), the source light including source comb frequencies (OCF) with a source frequency spacing (RR), the coupled light including an interval of frequencies centered on a main frequency of said comb frequencies due to cavity dispersion; -Locking the waveguide optical cavity to the frequency comb at said main optical frequency; -Detecting transmitted cavity frequencies; -Determining absorption by said sample (S) of said main optical frequency from the detected transmitted frequencies, -Changing the cavity mode frequency (FSR) spacing or the source frequency spacing (RR); -Coupling the pulse light to the waveguide optical cavity (3), the coupled light including an interval of frequencies centered on a second main frequency of said comb frequencies due to cavity dispersion;; -Locking the waveguide optical cavity to the frequency comb at said second main optical frequency; -Detecting transmitted cavity frequencies; -Determining absorption by said sample of said second main optical frequency from the detected transmitted frequencies.
    • 本发明涉及一种执行频率梳状光谱的方法和装置。 该方法包括: - 布置具有腔模式频率间隔(FSR)的多个腔模式频率的波导光腔(3),所述波导光腔是分散的,使得腔模的频率间隔是波长相关的; - 相对于所述波导光腔(3)布置样品(S),使得所述样品能够吸收行进到所述波导光腔中的光; 将来自光源(1)的脉冲光耦合到波导光腔(3)中,源光包括源频率间隔(RR)的源梳状频率(OCF),耦合光包括以 所述梳状频率由于腔体分散的主频率; 将所述波导光腔锁定在所述主光学频率处的频率梳; 检测发射的腔体频率; - 从所检测的发射频率确定所述主光频的所述采样(S)的吸收, - 使空腔模式频率(FSR)间隔或源频间隔(RR)延长; - 将所述脉冲光耦合到所述波导光腔(3),所述耦合光包括由于空腔分散而以所述梳状频率的第二主频率为中心的频率间隔; 将所述波导光腔锁定在所述第二主光学频率处的频率梳; 检测发射的腔体频率; - 从所检测的发射频率确定所述第二主光学频率的所述样本的吸收。
    • 8. 发明申请
    • METHOD FOR THE PRODUCTION OF A VISIBLE, UV OR IR RADIATION WITH A LAMP WITHOUT ELECTRODES, AND LAMP THAT CARRIES OUT THIS METHOD
    • 使用无电极产生可见光,紫外或红外辐射的方法,以及符合本方法的灯
    • WO2003047318A1
    • 2003-06-05
    • PCT/IB2002/005004
    • 2002-11-29
    • CNR CONSIGLIO NAZIONALE DELLE RICERCHELONGO, Iginio
    • LONGO, Iginio
    • H05B41/24
    • H05B41/24H01J65/044
    • A lamp capable of emitting electromagnetic radiation (9), for example visible, IR or UV radiation, exploiting the activation of substances (4) triggered with an antenna (6) irradiating microwaves (8) located inside and insulated, in focal position. Advantageously, the substances (4) are put into a chamber (3) obtained by introduction of a first bulb (1) in a second bulb, in order to form the chamber (3) closed between the walls of first (1) and of the second bulb (2), the walls of the first bulb defining the recess (5) which houses the antenna (6). A better energy efficiency and a better economy is obtained with respect to the conventional techniques which require introduction of the lamp in a metal vessel crossed by microwaves, or under external microwaves beams. It belongs to the category of lamps without electrodes, because the atoms or the other particles that emit the radiation (8) are neither in contact with the antenna nor with other metal parts. It characterized by a high duration and by the possibility of emitting radiation of modulated wavelength in continuous or pulsed way.
    • 一种能够发射电磁辐射(9)的灯(例如可见的,IR或UV辐射),利用辐射位于焦点位置内部并绝缘的微波(8)的天线(6)触发的物质(4)的激活。 有利地,将物质(4)放入通过将第一灯泡(1)引入第二灯泡而获得的室(3)中,以形成在第一(1)的壁之间封闭的室(3)和 第二灯泡(2),第一灯泡的壁限定容纳天线(6)的凹部(5)。 对于需要在由微波穿过的金属容器中或在外部微波束下引入灯的常规技术,可获得更好的能量效率和更好的经济性。 它属于没有电极的灯的类别,因为发射辐射(8)的原子或其他颗粒既不与天线接触也不与其它金属部件接触。 其特征在于持续时间高,并且以连续或脉冲方式发射调制波长的辐射的可能性。
    • 9. 发明申请
    • STRUCTURE OF INTEGRATED PHOTOCHEMICAL REACTOR
    • 一体化光电反应器结构
    • WO2016151439A1
    • 2016-09-29
    • PCT/IB2016/051502
    • 2016-03-17
    • CNR - CONSIGLIO NAZIONALE DELLE RICERCHE
    • LONGO, IginioFERRARI, Carlo
    • B01J19/08B01J19/12
    • B01J19/088B01J19/124B01J19/126B01J19/127B01J19/128B01J19/2425B01J19/243B01J19/2435B01J2219/0871B01J2219/0894B01J2219/1215B01J2219/1227B01J2219/1242B01J2219/1293B01J2219/1296H01J65/044
    • A structure of photochemical reactor (1) comprises a hollow container body (10) having a side wall (11) made of a material arranged to contain an excited luminous plasma with electromagnetic fields and defining a closed excitation chamber (12) in which, in use, an excitable material (15) is present in such a way to obtain a discharge of the excited luminous plasma by microwave irradiation. The hollow container body (10) is provided with at least a hollow (20) that protrudes into the excitation chamber (12) and at least a microwave radiation source positioned, in use, in the hollow (20), and arranged to emit radiations in such a way to excite the excitable material (15) producing a luminous plasma. The structure of photochemical reactor (1) comprises, furthermore, a reaction tube (30) which, in use, passes through the excitation chamber (12) in such a way to be immersed in the luminous plasma. The reaction tube (30) is arranged to contain, in use, predetermined chemical reagents (35) and is made of a material that is transparent to the predetermined optical radiation emitted by the luminous plasma, in such a way that the optical radiation is arranged to hit the chemical reagents (35) for inducing the predetermined photochemical reaction
    • 光化学反应器(1)的结构包括具有侧壁(11)的中空容器体(10),所述侧壁由材料构成,所述侧壁被布置成容纳具有电磁场的激发的发光等离子体并限定封闭的激发室(12),其中, 使用时,以这样的方式存在可兴奋材料(15),以通过微波照射获得激发的发光等离子体的放电。 中空容器主体(10)至少设置有一个突出到激励室(12)中的中空(20)和至少一个在使用中定位在中空(20)中的微波辐射源,并且被布置成发射辐射 以这种方式激发产生发光等离子体的可兴奋材料(15)。 此外,光化学反应器(1)的结构还包括在使用中通过激发室(12)以浸入发光等离子体的方式的反应管(30)。 反应管(30)被设置为在使用中包含预定的化学试剂(35),并且由对发光等离子体发射的预定光辐射透明的材料制成,使得光辐射被布置 击中化学试剂(35)以诱导预定的光化学反应
    • 10. 发明申请
    • HIGH VOLTAGE FIBER OPTIC SENSOR FOR THE MEASUREMENT OF AN ALTERNATING ELECTRIC FIELD
    • 用于测量交流电场的高压光纤传感器
    • WO2015052294A1
    • 2015-04-16
    • PCT/EP2014/071694
    • 2014-10-09
    • CNR-CONSIGLIO NAZIONALE DELLE RICERCHELEDA SRL, LABORATORIO DI ELETTRODINAMICA AVANZATA
    • GAGLIARDI, GianlucaMARIGNETTI, Fabrizio
    • G01R15/24
    • G01R15/24G01R29/12
    • The present invention is relative to a method to measure an alternating electric field, wherein said method includes: Realizing a first diffraction grating (1) in a first location, in a core of a silica-based optical fiber (2); Measuring the peak reflection wavelength of said first diffraction grating (1); positioning said optical fiber (2) along a direction having a non-zero component of an electrical field generated by an alternating voltage to be measured; coupling a substantially monochromatic light to said optical fiber (2) surrounded by said electric field; Measuring a parameter dependent on the shift of said peak reflection wavelength due to intrinsic mechanical deformation or refractive index change of the material in which said optical fiber (2) and said diffracting grating are realized due to the alternating electric field to which the material itself in which the optical fiber and diffraction grating are realized is subjected to; and Calculating a value of the electric field causing such a measured deformation or refractive index change.
    • 本发明涉及一种测量交变电场的方法,其中所述方法包括:在第二位置,在二氧化硅基光纤(2)的芯中实现第一衍射光栅(1); 测量所述第一衍射光栅(1)的峰值反射波长; 沿着具有由待测量的交流电压产生的电场的非零分量的方向定位所述光纤(2); 将基本上单色的光耦合到由所述电场包围的所述光纤(2); 由于材料自身的交变电场而实现由于所述光纤(2)和所述衍射光栅的材料的固有机械变形或材料的折射率变化而导致的所述峰值反射波长的偏移的参数的测量, 实现光纤和衍射光栅的实现; 并计算引起这种测量的变形或折射率变化的电场的值。