公开(公告)号：WO2010058432A8

公开(公告)日：2011-05-26

申请号：PCT/IT2008000724

申请日：2008-11-24

Applicant: SELEX SISTEMI INTEGRATI SPA ,  BOVINO FABIO ANTONIO ,  GIARDINA MAURIZIO ,  LARCIPRETE MARIA CRISTINA ,  CENTINI MARCO ,  BELARDINI ALESSANDRO ,  SIBILIA CONCITA ,  BERTOLOTTI MARIO ,  PASSASEO ADRIANA ,  TASCO VITTORIANNA ,  CINGOLANI ROBERTO

Inventor： BOVINO FABIO ANTONIO ,  GIARDINA MAURIZIO ,  LARCIPRETE MARIA CRISTINA ,  CENTINI MARCO ,  BELARDINI ALESSANDRO ,  SIBILIA CONCITA ,  BERTOLOTTI MARIO ,  PASSASEO ADRIANA ,  TASCO VITTORIANNA ,  CINGOLANI ROBERTO

IPC: G02F1/37 ,  G02F3/00

CPC classification number: G02F1/37 ,  G02F1/3534 ,  G02F3/00 ,  G02F2202/10

Abstract: Optical logic gate (1) having a second -harmonic generator element (15) that receives a first (sii) and a second optical input signal (si2) respectively having a first (?1) and a second angular frequency (?2) and respectively having a first (P; S) and a second (P; S) polarization, and which provides a second-harmonic optical signal (su3) having a third angular frequency (2?i, ?1+?2) and a third (P; S) polarization. The third angular frequency (2?i, ?1+?2) is equal to the sum of the first (?1) and the second angular frequency (?2). The third (P; S) polarization is a function of the first (P; S) and the second (P; S) polarization. The second-harmonic generator element (15) includes a second-harmonic generator layer (22) in a material having a non-null second-order optical tensor.

Abstract translation: 具有接收分别具有第一（θ1）和第二角频率（ω2）的第一（sii）和第二光输入信号（si2）的第二 - 谐波发生器元件（15）的光逻辑门（1）; 分别具有第一（P; S）和第二（P; S）偏振，并且提供具有第三角频率（2πi，θ1+λ2）的第二谐波光信号（su3） （P; S）极化。 第三角频率（2πi，ψ1+ρ2）等于第一（θ1）和第二角频率（ω2）的和。 第三（P; S）偏振是第一（P; S）和第二（P; S）偏振的函数。 二次谐波发生器元件（15）包括具有非零二阶光学张量的材料中的二次谐波发生器层（22）。

公开(公告)号：WO2010058432A1

公开(公告)日：2010-05-27

申请号：PCT/IT2008/000724

申请日：2008-11-24

Applicant: ELSAG DATAMAT SPA ,  BOVINO, Fabio Antonio ,  GIARDINA, Maurizio ,  LARCIPRETE, Maria Cristina ,  CENTINI, Marco ,  BELARDINI, Alessandro ,  SIBILIA, Concita ,  BERTOLOTTI, Mario ,  PASSASEO, Adriana ,  TASCO, Vittorianna ,  CINGOLANI, Roberto

Inventor： BOVINO, Fabio Antonio ,  GIARDINA, Maurizio ,  LARCIPRETE, Maria Cristina ,  CENTINI, Marco ,  BELARDINI, Alessandro ,  SIBILIA, Concita ,  BERTOLOTTI, Mario ,  PASSASEO, Adriana ,  TASCO, Vittorianna ,  CINGOLANI, Roberto

IPC: G02F1/37 ,  G02F3/00

CPC classification number: G02F1/37 ,  G02F1/3534 ,  G02F3/00 ,  G02F2202/10

Abstract: Optical logic gate (1) having a second -harmonic generator element (15) that receives a first (s ii ) and a second optical input signal (s i2 ) respectively having a first (ω 1 ) and a second angular frequency (ω 2 ) and respectively having a first (P; S) and a second (P; S) polarization, and which provides a second-harmonic optical signal (s u3 ) having a third angular frequency (2ω i , ω 1 +ω 2 ) and a third (P; S) polarization. The third angular frequency (2ω i , ω 1 +ω 2 ) is equal to the sum of the first (ω 1 ) and the second angular frequency (ω 2 ). The third (P; S) polarization is a function of the first (P; S) and the second (P; S) polarization. The second-harmonic generator element (15) includes a second-harmonic generator layer (22) in a material having a non-null second-order optical tensor.

Abstract translation: 具有接收分别具有第一（λ1）和第二角频率（ω2）的第一（sii）和第二光输入信号（si2）的第二和谐发生器元件（15）的光逻辑门（1）和 分别具有第一（P; S）和第二（P; S）极化，并且其提供具有第三角频率（2πi，ω1+α2）和第三 （P; S）极化。 第三角频率（2πi，ω1+θ2）等于第一（α1）和第二角频率（ω2）之和。 第三（P; S）极化是第一（P; S）和第二（P; S）极化的函数。 二次谐波发生器元件（15）包括具有非零二次光张张的材料中的二次谐波发生器层（22）。

公开(公告)号：WO2010113190A8

公开(公告)日：2011-01-27

申请号：PCT/IT2009000131

申请日：2009-03-31

Applicant: SELEX SISTEMI INTEGRATI SPA ,  BOVINO FABIO ANTONIO ,  LARCIPRETE MARIA CRISTINA ,  GIARDINA MAURIZIO ,  SIBILIA CONCITA

Inventor： BOVINO FABIO ANTONIO ,  LARCIPRETE MARIA CRISTINA ,  GIARDINA MAURIZIO ,  SIBILIA CONCITA

IPC: G02F1/35 ,  G01N21/63

CPC classification number: G02F1/3532 ,  G01N21/21 ,  G01N21/41 ,  G01N21/636

Abstract: Described herein is a method for determining second- order nonlinear optical coefficients of a material. The method envisages the steps of providing a specimen (1;35) made at least in part of the material, causing a first optical signal (Si1) and a second optical signal (Si2) having, respectively, a first pulsation and a second pulsation, and a first polarization state and a second polarization state, to impinge upon the specimen in such a way that the specimen generates a second-harmonic optical signal (su3) having a third pulsation equal to the sum of the first and second pulsations, and a third polarization state that is a function of the first and second polarization states. The method further envisages the step of determining a plurality of measurements of power corresponding to the second-harmonic optical signal, and the step of determining the second-order nonlinear optical coefficients on the basis of the plurality of measurements of power. In addition, the method envisages performing a plurality of measurements of power of the second-harmonic optical signal as the first polarization state and the second polarization state vary.

Abstract translation: 这里描述了一种用于确定材料的二阶非线性光学系数的方法。 该方法设想提供至少部分材料制成的样品（1; 35）的步骤，产生分别具有第一脉动和第二脉动的第一光信号（Si1）和第二光信号（Si2） 以及第一偏振态和第二偏振态，以使样本产生具有等于第一和第二脉动的和的第三脉动的二次谐波光信号（su3）的方式撞击在样本上，以及 第三极化状态，其是第一和第二极化状态的函数。 该方法进一步设想了确定对应于二次谐波光信号的多个功率测量的步骤，以及基于多次功率测量来确定二阶非线性光学系数的步骤。 此外，该方法设想当第一偏振态和第二极化状态变化时执行二次谐波光信号的功率的多个测量。

公开(公告)号：WO2010113190A1

公开(公告)日：2010-10-07

申请号：PCT/IT2009/000131

申请日：2009-03-31

Applicant: ELSAG DATAMAT SPA ,  BONVINO, Fabio Antonio ,  LARCIPRETE, Maria Cristina ,  GIARDINA, Maurizio ,  SIBILIA, Concita

Inventor： BONVINO, Fabio Antonio ,  LARCIPRETE, Maria Cristina ,  GIARDINA, Maurizio ,  SIBILIA, Concita

IPC: G02F1/35 ,  G01N21/63

CPC classification number: G02F1/3532 ,  G01N21/21 ,  G01N21/41 ,  G01N21/636

Abstract: Described herein is a method for determining second- order nonlinear optical coefficients of a material. The method envisages the steps of providing a specimen (1;35) made at least in part of the material, causing a first optical signal (S i1 ) and a second optical signal (S i2 ) having, respectively, a first pulsation and a second pulsation, and a first polarization state and a second polarization state, to impinge upon the specimen in such a way that the specimen generates a second-harmonic optical signal (s u3 ) having a third pulsation equal to the sum of the first and second pulsations, and a third polarization state that is a function of the first and second polarization states. The method further envisages the step of determining a plurality of measurements of power corresponding to the second-harmonic optical signal, and the step of determining the second-order nonlinear optical coefficients on the basis of the plurality of measurements of power. In addition, the method envisages performing a plurality of measurements of power of the second-harmonic optical signal as the first polarization state and the second polarization state vary.

Abstract translation: 这里描述了一种用于确定材料的二阶非线性光学系数的方法。 该方法设想提供至少部分材料制成的样品（1; 35）的步骤，产生分别具有第一脉动和第二脉动的第一光信号（Si1）和第二光信号（Si2） 以及第一偏振态和第二偏振态，以使得样本产生具有等于第一和第二脉动之和的第三脉动的二次谐波光信号（su3）的方式撞击在样本上，以及 第三极化状态，其是第一和第二极化状态的函数。 该方法进一步设想了确定对应于二次谐波光信号的多个功率测量的步骤，以及基于多个功率测量来确定二阶非线性光学系数的步骤。 此外，该方法设想当第一偏振态和第二极化状态变化时执行二次谐波光信号的功率的多个测量。

公开(公告)号：WO2010058432A9

公开(公告)日：2011-07-07

申请号：PCT/IT2008000724

申请日：2008-11-24

Applicant: SELEX SISTEMI INTEGRATI SPA ,  BOVINO FABIO ANTONIO ,  GIARDINA MAURIZIO ,  LARCIPRETE MARIA CRISTINA ,  CENTINI MARCO ,  BELARDINI ALESSANDRO ,  SIBILIA CONCITA ,  BERTOLOTTI MARIO ,  PASSASEO ADRIANA ,  TASCO VITTORIANNA ,  CINGOLANI ROBERTO

Inventor： BOVINO FABIO ANTONIO ,  GIARDINA MAURIZIO ,  LARCIPRETE MARIA CRISTINA ,  CENTINI MARCO ,  BELARDINI ALESSANDRO ,  SIBILIA CONCITA ,  BERTOLOTTI MARIO ,  PASSASEO ADRIANA ,  TASCO VITTORIANNA ,  CINGOLANI ROBERTO

IPC: G02F1/37 ,  G02F3/00

CPC classification number: G02F1/37 ,  G02F1/3534 ,  G02F3/00 ,  G02F2202/10

Abstract: Optical logic gate (1) having a second -harmonic generator element (15) that receives a first (sii) and a second optical input signal (si2) respectively having a first (?1) and a second angular frequency (?2) and respectively having a first (P; S) and a second (P; S) polarization, and which provides a second-harmonic optical signal (su3) having a third angular frequency (2?i, ?1+?2) and a third (P; S) polarization. The third angular frequency (2?i, ?1+?2) is equal to the sum of the first (?1) and the second angular frequency (?2). The third (P; S) polarization is a function of the first (P; S) and the second (P; S) polarization. The second-harmonic generator element (15) includes a second-harmonic generator layer (22) in a material having a non-null second-order optical tensor.

Abstract translation: 具有接收分别具有第一（λ1）和第二角频率（ω2）的第一（sii）和第二光输入信号（si2）的第二和谐发生器元件（15）的光逻辑门（1）和 分别具有第一（P; S）和第二（P; S）极化，并且其提供具有第三角频率（2πi，ω1+α2）和第三 （P; S）极化。 第三角频率（2πi，ω1+θ2）等于第一（α1）和第二角频率（ω2）之和。 第三（P; S）极化是第一（P; S）和第二（P; S）极化的函数。 二次谐波发生器元件（15）包括具有非零二次光张张的材料中的二次谐波发生器层（22）。